Measurements of observables sensitive to colour reconnection in $t\bar{t}$ events with the ATLAS detector at $\sqrt{s}=13$ TeV

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abbott, D.C. ; et al.
Eur.Phys.J.C 83 (2023) 518, 2023.
Inspire Record 2152933 DOI 10.17182/hepdata.135459

A measurement of observables sensitive to effects of colour reconnection in top-quark pair-production events is presented using 139 fb$^{-1}$ of 13$\,$TeV proton-proton collision data collected by the ATLAS detector at the LHC. Events are selected by requiring exactly one isolated electron and one isolated muon with opposite charge and two or three jets, where exactly two jets are required to be $b$-tagged. For the selected events, measurements are presented for the charged-particle multiplicity, the scalar sum of the transverse momenta of the charged particles, and the same scalar sum in bins of charged-particle multiplicity. These observables are unfolded to the stable-particle level, thereby correcting for migration effects due to finite detector resolution, acceptance and efficiency effects. The particle-level measurements are compared with different colour reconnection models in Monte Carlo generators. These measurements disfavour some of the colour reconnection models and provide inputs to future optimisation of the parameters in Monte Carlo generators.

149 data tables

Binning used for the measured $\sum_{n_{\text{ch}}} p_{\text{T}}$ in bins of $n_\text{ch}$ observable.

Event yields obtained after the event selection. The expected event yields from $t\bar{t}$ production and the various background processes are compared with the observed event yield. The fractional contributions from $t\bar{t}$ production and the background processes to the expected event yield is given in %. The processes labelled by `Others' include production of $Z$+jets and diboson background events. The uncertainties include the MC statistical uncertainty and the normalisation uncertainty.

Summary of the estimated pile-up scale factors $c_{\text{PU}}$, parameterisd in $\mu$ and $n_{\text{trk,out}}$. All values have a statistical precision of 0.01.

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Version 2
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at $\sqrt{s}=13$ TeV

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abbott, Dale ; et al.
JHEP 06 (2022) 063, 2022.
Inspire Record 2037744 DOI 10.17182/hepdata.134011

Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than $355$ GeV and the other top quark decays into $\ell \nu b$ are presented using 139 fb$^{-1}$ of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at $\sqrt{s}=13$ TeV is measured to be $\sigma = 1.267 \pm 0.005 \pm 0.053$ pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of $4.2\%$. The cross-section is measured differentially as a function of variables characterising the $t\bar{t}$ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to set limits on the Wilson coefficients of the dimension-six operators $O_{tG}$ and $O_{tq}^{(8)}$ in the effective field theory framework.

275 data tables

- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definitions:</b><br/> <ul> <li> NLEP = 1, either E or MU, PT &gt; 27 GeV, ABS ETA &lt; 2.5 <li> NJETS &gt;= 2, R = 0.4, PT &gt; 26 GeV, ABS ETA &lt; 2.5 <li> NBJETS &gt;= 2 <li> NJETS &gt;= 1, R=1, PT &gt; 355 GeV, ABS ETA &lt; 2.0, top-tagged </ul><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>SIG (<a href="1651136742?version=1&table=Table 1">Table 1</a> ) <li>DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 2">Table 2</a> ) <li>1/SIG*DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 4">Table 4</a> ) <li>DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 5">Table 5</a> ) <li>1/SIG*DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 7">Table 7</a> ) <li>DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 8">Table 8</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 10">Table 10</a> ) <li>DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 11">Table 11</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 13">Table 13</a> ) <li>DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 14">Table 14</a> ) <li>1/SIG*DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 16">Table 16</a> ) <li>DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 17">Table 17</a> ) <li>1/SIG*DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 19">Table 19</a> ) <li>DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 20">Table 20</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 22">Table 22</a> ) <li>DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 23">Table 23</a> ) <li>1/SIG*DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 25">Table 25</a> ) <li>DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 26">Table 26</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 28">Table 28</a> ) <li>DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 29">Table 29</a> ) <li>1/SIG*DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 31">Table 31</a> ) <li>DSIG/DHT (<a href="1651136742?version=1&table=Table 32">Table 32</a> ) <li>1/SIG*DSIG/DHT (<a href="1651136742?version=1&table=Table 34">Table 34</a> ) <li>DSIG/DNJETS (<a href="1651136742?version=1&table=Table 35">Table 35</a> ) <li>1/SIG*DSIG/DNJETS (<a href="1651136742?version=1&table=Table 37">Table 37</a> ) <li>DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 38">Table 38</a> ) <li>1/SIG*DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 40">Table 40</a> ) <li>DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 41">Table 41</a> ) <li>1/SIG*DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 43">Table 43</a> ) <li>DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 44">Table 44</a> ) <li>1/SIG*DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 46">Table 46</a> ) <li>DSIG/DDPHIOPI_THAD_J2 (<a href="1651136742?version=1&table=Table 47">Table 47</a> ) <li>1/SIG*DSIG/DDPHIOPI_THAD_J2 (<a href="1651136742?version=1&table=Table 49">Table 49</a> ) <li>DSIG/DDPHIOPI_J1_J2 (<a href="1651136742?version=1&table=Table 50">Table 50</a> ) <li>1/SIG*DSIG/DDPHIOPI_J1_J2 (<a href="1651136742?version=1&table=Table 52">Table 52</a> ) <li>DSIG/DPT_J2 (<a href="1651136742?version=1&table=Table 53">Table 53</a> ) <li>1/SIG*DSIG/DPT_J2 (<a href="1651136742?version=1&table=Table 55">Table 55</a> ) </ul><br/> Statistical covariance matrices: <ul> <li>DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 3">Table 3</a> ) <li>DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 6">Table 6</a> ) <li>DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 9">Table 9</a> ) <li>DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 12">Table 12</a> ) <li>DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 15">Table 15</a> ) <li>DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 18">Table 18</a> ) <li>DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 21">Table 21</a> ) <li>DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 24">Table 24</a> ) <li>DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 27">Table 27</a> ) <li>DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 30">Table 30</a> ) <li>DSIG/DHT (<a href="1651136742?version=1&table=Table 33">Table 33</a> ) <li>DSIG/DNJETS (<a href="1651136742?version=1&table=Table 36">Table 36</a> ) <li>DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 39">Table 39</a> ) <li>DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 42">Table 42</a> ) <li>DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 45">Table 45</a> ) <li>DSIG/DDPHIOPI_THAD_J2 (<a href="1651136742?version=1&table=Table 48">Table 48</a> ) <li>DSIG/DDPHIOPI_J1_J2 (<a href="1651136742?version=1&table=Table 51">Table 51</a> ) <li>DSIG/DPT_J2 (<a href="1651136742?version=1&table=Table 54">Table 54</a> ) </ul><br/> Inter-spectra statistical covariance matrices: <ul> <li>Statistical covariance between DSIG/DPT_THAD and DSIG/DSIG (<a href="1651136742?version=1&table=Table 104">Table 104</a> ) <li>Statistical covariance between DSIG/DPT_TLEP and DSIG/DSIG (<a href="1651136742?version=1&table=Table 105">Table 105</a> ) <li>Statistical covariance between DSIG/DPT_TLEP and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 106">Table 106</a> ) <li>Statistical covariance between DSIG/DM_TTBAR and DSIG/DSIG (<a href="1651136742?version=1&table=Table 107">Table 107</a> ) <li>Statistical covariance between DSIG/DM_TTBAR and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 108">Table 108</a> ) <li>Statistical covariance between DSIG/DM_TTBAR and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 109">Table 109</a> ) <li>Statistical covariance between DSIG/DABS_Y_THAD and DSIG/DSIG (<a href="1651136742?version=1&table=Table 110">Table 110</a> ) <li>Statistical covariance between DSIG/DABS_Y_THAD and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 111">Table 111</a> ) <li>Statistical covariance between DSIG/DABS_Y_THAD and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 112">Table 112</a> ) <li>Statistical covariance between DSIG/DABS_Y_THAD and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 113">Table 113</a> ) <li>Statistical covariance between DSIG/DABS_Y_TLEP and DSIG/DSIG (<a href="1651136742?version=1&table=Table 114">Table 114</a> ) <li>Statistical covariance between DSIG/DABS_Y_TLEP and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 115">Table 115</a> ) <li>Statistical covariance between DSIG/DABS_Y_TLEP and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 116">Table 116</a> ) <li>Statistical covariance between DSIG/DABS_Y_TLEP and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 117">Table 117</a> ) <li>Statistical covariance between DSIG/DABS_Y_TLEP and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 118">Table 118</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DSIG (<a href="1651136742?version=1&table=Table 119">Table 119</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 120">Table 120</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 121">Table 121</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 122">Table 122</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 123">Table 123</a> ) <li>Statistical covariance between DSIG/DY_TTBAR and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 124">Table 124</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DSIG (<a href="1651136742?version=1&table=Table 125">Table 125</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 126">Table 126</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 127">Table 127</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 128">Table 128</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 129">Table 129</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 130">Table 130</a> ) <li>Statistical covariance between DSIG/DHT_TTBAR and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 131">Table 131</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DSIG (<a href="1651136742?version=1&table=Table 132">Table 132</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 133">Table 133</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 134">Table 134</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 135">Table 135</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 136">Table 136</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 137">Table 137</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 138">Table 138</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_BLEP and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 139">Table 139</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DSIG (<a href="1651136742?version=1&table=Table 140">Table 140</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 141">Table 141</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 142">Table 142</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 143">Table 143</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 144">Table 144</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 145">Table 145</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 146">Table 146</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 147">Table 147</a> ) <li>Statistical covariance between DSIG/DPT_TTBAR and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 148">Table 148</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DSIG (<a href="1651136742?version=1&table=Table 149">Table 149</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 150">Table 150</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 151">Table 151</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 152">Table 152</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 153">Table 153</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 154">Table 154</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 155">Table 155</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 156">Table 156</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 157">Table 157</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_TTBAR and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 158">Table 158</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DSIG (<a href="1651136742?version=1&table=Table 159">Table 159</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 160">Table 160</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 161">Table 161</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 162">Table 162</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 163">Table 163</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 164">Table 164</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 165">Table 165</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 166">Table 166</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 167">Table 167</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 168">Table 168</a> ) <li>Statistical covariance between DSIG/DHT and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 169">Table 169</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DSIG (<a href="1651136742?version=1&table=Table 170">Table 170</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 171">Table 171</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 172">Table 172</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 173">Table 173</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 174">Table 174</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 175">Table 175</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 176">Table 176</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 177">Table 177</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 178">Table 178</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 179">Table 179</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 180">Table 180</a> ) <li>Statistical covariance between DSIG/DNJETS and DSIG/DHT (<a href="1651136742?version=1&table=Table 181">Table 181</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DSIG (<a href="1651136742?version=1&table=Table 182">Table 182</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 183">Table 183</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 184">Table 184</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 185">Table 185</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 186">Table 186</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 187">Table 187</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 188">Table 188</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 189">Table 189</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 190">Table 190</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 191">Table 191</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 192">Table 192</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DHT (<a href="1651136742?version=1&table=Table 193">Table 193</a> ) <li>Statistical covariance between DSIG/DPT_J1 and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 194">Table 194</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DSIG (<a href="1651136742?version=1&table=Table 195">Table 195</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 196">Table 196</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 197">Table 197</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 198">Table 198</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 199">Table 199</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 200">Table 200</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 201">Table 201</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 202">Table 202</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 203">Table 203</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 204">Table 204</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 205">Table 205</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DHT (<a href="1651136742?version=1&table=Table 206">Table 206</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 207">Table 207</a> ) <li>Statistical covariance between DSIG/DM_J1_THAD and DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 208">Table 208</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DSIG (<a href="1651136742?version=1&table=Table 209">Table 209</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 210">Table 210</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 211">Table 211</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 212">Table 212</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 213">Table 213</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 214">Table 214</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 215">Table 215</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 216">Table 216</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 217">Table 217</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 218">Table 218</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 219">Table 219</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DHT (<a href="1651136742?version=1&table=Table 220">Table 220</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 221">Table 221</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 222">Table 222</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J1 and DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 223">Table 223</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DSIG (<a href="1651136742?version=1&table=Table 224">Table 224</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 225">Table 225</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 226">Table 226</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 227">Table 227</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 228">Table 228</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 229">Table 229</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 230">Table 230</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 231">Table 231</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 232">Table 232</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 233">Table 233</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 234">Table 234</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DHT (<a href="1651136742?version=1&table=Table 235">Table 235</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 236">Table 236</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 237">Table 237</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 238">Table 238</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_THAD_J2 and DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 239">Table 239</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DSIG (<a href="1651136742?version=1&table=Table 240">Table 240</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 241">Table 241</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 242">Table 242</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 243">Table 243</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 244">Table 244</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 245">Table 245</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 246">Table 246</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 247">Table 247</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 248">Table 248</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 249">Table 249</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 250">Table 250</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DHT (<a href="1651136742?version=1&table=Table 251">Table 251</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 252">Table 252</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 253">Table 253</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 254">Table 254</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 255">Table 255</a> ) <li>Statistical covariance between DSIG/DDPHIOPI_J1_J2 and DSIG/DDPHIOPI_THAD_J2 (<a href="1651136742?version=1&table=Table 256">Table 256</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DSIG (<a href="1651136742?version=1&table=Table 257">Table 257</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DPT_THAD (<a href="1651136742?version=1&table=Table 258">Table 258</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DPT_TLEP (<a href="1651136742?version=1&table=Table 259">Table 259</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DM_TTBAR (<a href="1651136742?version=1&table=Table 260">Table 260</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DABS_Y_THAD (<a href="1651136742?version=1&table=Table 261">Table 261</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DABS_Y_TLEP (<a href="1651136742?version=1&table=Table 262">Table 262</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DY_TTBAR (<a href="1651136742?version=1&table=Table 263">Table 263</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DHT_TTBAR (<a href="1651136742?version=1&table=Table 264">Table 264</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DDPHIOPI_THAD_BLEP (<a href="1651136742?version=1&table=Table 265">Table 265</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DPT_TTBAR (<a href="1651136742?version=1&table=Table 266">Table 266</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DDPHIOPI_TTBAR (<a href="1651136742?version=1&table=Table 267">Table 267</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DHT (<a href="1651136742?version=1&table=Table 268">Table 268</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DNJETS (<a href="1651136742?version=1&table=Table 269">Table 269</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DPT_J1 (<a href="1651136742?version=1&table=Table 270">Table 270</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DM_J1_THAD (<a href="1651136742?version=1&table=Table 271">Table 271</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DDPHIOPI_THAD_J1 (<a href="1651136742?version=1&table=Table 272">Table 272</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DDPHIOPI_THAD_J2 (<a href="1651136742?version=1&table=Table 273">Table 273</a> ) <li>Statistical covariance between DSIG/DPT_J2 and DSIG/DDPHIOPI_J1_J2 (<a href="1651136742?version=1&table=Table 274">Table 274</a> ) </ul><br/> <u>2D:</u><br/> Spectra: <ul> <li>1/SIG*D2SIG/DPT_J1/DNJETS (NJETS = 1) (<a href="1651136742?version=1&table=Table 56">Table 56</a> ) <li>1/SIG*D2SIG/DPT_J1/DNJETS (NJETS = 2) (<a href="1651136742?version=1&table=Table 57">Table 57</a> ) <li>1/SIG*D2SIG/DPT_J1/DNJETS (NJETS $\geq$ 3) (<a href="1651136742?version=1&table=Table 58">Table 58</a> ) <li>D2SIG/DPT_J1/DNJETS (NJETS = 1) (<a href="1651136742?version=1&table=Table 59">Table 59</a> ) <li>D2SIG/DPT_J1/DNJETS (NJETS = 2) (<a href="1651136742?version=1&table=Table 60">Table 60</a> ) <li>D2SIG/DPT_J1/DNJETS (NJETS $\geq$ 3) (<a href="1651136742?version=1&table=Table 61">Table 61</a> ) <li>1/SIG*D2SIG/DPT_J1/DPT_THAD ( 355.0 GeV < PT_THAD < 398.0 GeV) (<a href="1651136742?version=1&table=Table 68">Table 68</a> ) <li>1/SIG*D2SIG/DPT_J1/DPT_THAD ( 398.0 GeV < PT_THAD < 496.0 GeV) (<a href="1651136742?version=1&table=Table 69">Table 69</a> ) <li>1/SIG*D2SIG/DPT_J1/DPT_THAD ( 496.0 GeV < PT_THAD < 2000.0 GeV) (<a href="1651136742?version=1&table=Table 70">Table 70</a> ) <li>D2SIG/DPT_J1/DPT_THAD ( 355.0 GeV < PT_THAD < 398.0 GeV) (<a href="1651136742?version=1&table=Table 71">Table 71</a> ) <li>D2SIG/DPT_J1/DPT_THAD ( 398.0 GeV < PT_THAD < 496.0 GeV) (<a href="1651136742?version=1&table=Table 72">Table 72</a> ) <li>D2SIG/DPT_J1/DPT_THAD ( 496.0 GeV < PT_THAD < 2000.0 GeV) (<a href="1651136742?version=1&table=Table 73">Table 73</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 355.0 GeV < PT_THAD < 398.0 GeV) (<a href="1651136742?version=1&table=Table 80">Table 80</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 398.0 GeV < PT_THAD < 496.0 GeV) (<a href="1651136742?version=1&table=Table 81">Table 81</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 496.0 GeV < PT_THAD < 2000.0 GeV) (<a href="1651136742?version=1&table=Table 82">Table 82</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 355.0 GeV < PT_THAD < 398.0 GeV) (<a href="1651136742?version=1&table=Table 83">Table 83</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 398.0 GeV < PT_THAD < 496.0 GeV) (<a href="1651136742?version=1&table=Table 84">Table 84</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DPT_THAD ( 496.0 GeV < PT_THAD < 2000.0 GeV) (<a href="1651136742?version=1&table=Table 85">Table 85</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS = 1) (<a href="1651136742?version=1&table=Table 92">Table 92</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS = 2) (<a href="1651136742?version=1&table=Table 93">Table 93</a> ) <li>1/SIG*D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS $\geq$ 3) (<a href="1651136742?version=1&table=Table 94">Table 94</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS = 1) (<a href="1651136742?version=1&table=Table 95">Table 95</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS = 2) (<a href="1651136742?version=1&table=Table 96">Table 96</a> ) <li>D2SIG/DDPHIOPI_THAD_J1/DNJETS (NJETS $\geq$ 3) (<a href="1651136742?version=1&table=Table 97">Table 97</a> ) </ul><br/> Statistical covariance matrices: <ul> <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 1st and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 62">Table 62</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 2nd and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 63">Table 63</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 2nd and 2nd bins of NJETS (<a href="1651136742?version=1&table=Table 64">Table 64</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 3rd and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 65">Table 65</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 3rd and 2nd bins of NJETS (<a href="1651136742?version=1&table=Table 66">Table 66</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DNJETS between the 3rd and 3rd bins of NJETS (<a href="1651136742?version=1&table=Table 67">Table 67</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 1st and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 74">Table 74</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 2nd and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 75">Table 75</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 2nd and 2nd bins of PT_THAD (<a href="1651136742?version=1&table=Table 76">Table 76</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 3rd and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 77">Table 77</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 3rd and 2nd bins of PT_THAD (<a href="1651136742?version=1&table=Table 78">Table 78</a> ) <li>Statistical covariance matrix for D2SIG/DPT_J1/DPT_THAD between the 3rd and 3rd bins of PT_THAD (<a href="1651136742?version=1&table=Table 79">Table 79</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 1st and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 86">Table 86</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 2nd and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 87">Table 87</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 2nd and 2nd bins of PT_THAD (<a href="1651136742?version=1&table=Table 88">Table 88</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 3rd and 1st bins of PT_THAD (<a href="1651136742?version=1&table=Table 89">Table 89</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 3rd and 2nd bins of PT_THAD (<a href="1651136742?version=1&table=Table 90">Table 90</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DPT_THAD between the 3rd and 3rd bins of PT_THAD (<a href="1651136742?version=1&table=Table 91">Table 91</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 1st and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 98">Table 98</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 2nd and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 99">Table 99</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 2nd and 2nd bins of NJETS (<a href="1651136742?version=1&table=Table 100">Table 100</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 3rd and 1st bins of NJETS (<a href="1651136742?version=1&table=Table 101">Table 101</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 3rd and 2nd bins of NJETS (<a href="1651136742?version=1&table=Table 102">Table 102</a> ) <li>Statistical covariance matrix for D2SIG/DDPHIOPI_THAD_J1/DNJETS between the 3rd and 3rd bins of NJETS (<a href="1651136742?version=1&table=Table 103">Table 103</a> ) </ul><br/>

Total cross-section at particle level in the boosted topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Absolute differential cross-section as a function of $p_T^{t,h}$ at particle level in the boosted topology. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

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Version 3
Measurement of the inclusive and differential $\mathrm{t\bar{t}}\gamma$ cross sections in the dilepton channel and effective field theory interpretation in proton-proton collisions at $\sqrt{s}$ =13 TeV

The CMS collaboration Tumasyan, Armen ; Adam, Wolfgang ; Andrejkovic, Janik Walter ; et al.
JHEP 05 (2022) 091, 2022.
Inspire Record 2013377 DOI 10.17182/hepdata.113657

The production cross section of a top quark pair in association with a photon is measured in proton-proton collisions in the decay channel with two oppositely charged leptons (e$^\pm\mu^\mp$, e$^+$e$^-$, or $\mu^+\mu^-$). The measurement is performed using 138 fb$^{-1}$ of proton-proton collision data recorded by the CMS experiment at $\sqrt{s} =$ 13 TeV during the 2016-2018 data-taking period of the CERN LHC. A fiducial phase space is defined such that photons radiated by initial-state particles, top quarks, or any of their decay products are included. An inclusive cross section of 175.2 $\pm$ 2.5 (stat) $\pm$ 6.3 (syst) fb is measured in a signal region with at least one jet coming from the hadronization of a bottom quark and exactly one photon with transverse momentum above 20 GeV. Differential cross sections are measured as functions of several kinematic observables of the photon, leptons, and jets, and compared to standard model predictions. The measurements are also interpreted in the standard model effective field theory framework, and limits are found on the relevant Wilson coefficients from these results alone and in combination with a previous CMS measurement of the $\mathrm{t\bar{t}}\gamma$ production process using the lepton+jets final state.

64 data tables

Observed and predicted event yields as a function of $p_{T}(\gamma)$ in the $e\mu$ channel, after the fit to the data.

Observed and predicted event yields as a function of $p_{T}(\gamma)$ in the $ee$ channel, after the fit to the data.

Observed and predicted event yields as a function of $p_{T}(\gamma)$ in the $\mu\mu$ channel, after the fit to the data.

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Version 2
Measurement of the inclusive and differential $\mathrm{t\overline{t}}\gamma$ cross sections in the single-lepton channel and EFT interpretation at $\sqrt{s}$ = 13 TeV

The CMS collaboration Tumasyan, Armen ; Adam, Wolfgang ; Andrejkovic, Janik Walter ; et al.
JHEP 12 (2021) 180, 2021.
Inspire Record 1876579 DOI 10.17182/hepdata.102876

The production cross section of a top quark pair in association with a photon is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The data set, corresponding to an integrated luminosity of 137 fb$^{-1}$, was recorded by the CMS experiment during the 2016-2018 data taking of the LHC. The measurements are performed in a fiducial volume defined at the particle level. Events with an isolated, highly energetic lepton, at least three jets from the hadronization of quarks, among which at least one is b tagged, and one isolated photon are selected. The inclusive fiducial $\mathrm{t\overline{t}}\gamma$ cross section, for a photon with transverse momentum greater than 20 GeV and pseudorapidity $\lvert \eta\rvert$$\lt$ 1.4442, is measured to be 798 $\pm$ 7 (stat) $\pm$ 48 (syst) fb, in good agreement with the prediction from the standard model at next-to-leading order in quantum chromodynamics. The differential cross sections are also measured as a function of several kinematic observables and interpreted in the framework of the standard model effective field theory (EFT), leading to the most stringent direct limits to date on anomalous electromagnetic dipole moment interactions of the top quark and the photon.

80 data tables

Distribution of $p_{T}(\gamma)$ in the $N_{jet}\geq 3$ signal region.

Distribution of $p_{T}(\gamma)$ in the $N_{jet}\geq 3$ signal region.

Distribution of $m_{T}(W)$ in the $N_{jet}\geq 3$ signal region.

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Version 2
Measurement of the $t\bar{t}$ production cross-section in the lepton+jets channel at $\sqrt{s}=13\;$TeV with the ATLAS experiment

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
Phys.Lett.B 810 (2020) 135797, 2020.
Inspire Record 1802524 DOI 10.17182/hepdata.95748

The $t\bar{t}$ production cross-section is measured in the lepton+jets channel using proton$-$proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 139 fb$^{-1}$. Events with exactly one charged lepton and four or more jets in the final state, with at least one jet containing $b$-hadrons, are used to determine the $t\bar{t}$ production cross-section through a profile-likelihood fit. The inclusive cross-section is measured to be ${\sigma_{\text{inc}} = 830 \pm 0.4~ \text{(stat.)}\pm 36~\text{(syst.)}\pm 14~\text{(lumi.)}~\mathrm{pb}}$ with a relative uncertainty of 4.6 %. The result is consistent with theoretical calculations at next-to-next-to-leading order in perturbative QCD. The fiducial $t\bar{t}$ cross-section within the experimental acceptance is also measured.

10 data tables

The results of fitted inclusive and fiducial ${t\bar{t}}$ cross-sections

The results of fitted inclusive and fiducial ${t\bar{t}}$ cross-sections

Ranking of the systematic uncertainties on the measured cross-section, normalised to the predicted value, in the inclusive fit to data. The impact of each nuisance parameter, $\Delta \sigma_{\text{inc}}/\sigma^{\text{pred.}}_{\text{inc}}$, is computed by comparing the nominal best-fit value of $\sigma_{\text{inc}}/\sigma^{\text{pred}}_{\text{inc}}$ with the result of the fit when fixing the considered nuisance parameter to its best-fit value, $\theta$, shifted by its pre-fit (post-fit) uncertainties $\pm \Delta \theta$ ($\pm \Delta \hat{\theta}$). The figure shows the effect of the ten most significant uncertainties.

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Measurements of top-quark pair single- and double-differential cross-sections in the all-hadronic channel in $pp$ collisions at $\sqrt{s}=13~\textrm{TeV}$ using the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
JHEP 01 (2021) 033, 2021.
Inspire Record 1801434 DOI 10.17182/hepdata.103063

Differential cross-sections are measured for top-quark pair production in the all-hadronic decay mode, using proton$-$proton collision events collected by the ATLAS experiment in which all six decay jets are separately resolved. Absolute and normalised single- and double-differential cross-sections are measured at particle and parton level as a function of various kinematic variables. Emphasis is placed on well-measured observables in fully reconstructed final states, as well as on the study of correlations between the top-quark pair system and additional jet radiation identified in the event. The study is performed using data from proton$-$proton collisions at $\sqrt{s}=13~\mbox{TeV}$ collected by the ATLAS detector at CERN's Large Hadron Collider in 2015 and 2016, corresponding to an integrated luminosity of $\mbox{36.1 fb}^{-1}$. The rapidities of the individual top quarks and of the top-quark pair are well modelled by several independent event generators. Significant mismodelling is observed in the transverse momenta of the leading three jet emissions, while the leading top-quark transverse momentum and top-quark pair transverse momentum are both found to be incompatible with several theoretical predictions.

674 data tables

- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definition:</b><br/> <ul> <li> NLEP = 0, either E or MU, PT &gt; 15 GeV, ABS ETA &lt; 1.37 <li> NJETS &gt;= 6, PT &gt; 25 GeV, ABS ETA &lt; 2.5 <li> NBJETS &gt;= 2 </ul><br/> <b>Particle level:</b><br/> <u>1D:</u><br/> Spectra: <ul> <li><a href="103063?version=1&table=Table 1">1/SIG*DSIG/DDR_E1J1</a> (Table 1) <li><a href="103063?version=1&table=Table 3">DSIG/DDR_E1J1</a> (Table 3) <li><a href="103063?version=1&table=Table 5">1/SIG*DSIG/DABS_T1_Y</a> (Table 5) <li><a href="103063?version=1&table=Table 7">DSIG/DABS_T1_Y</a> (Table 7) <li><a href="103063?version=1&table=Table 9">1/SIG*DSIG/DTT_M</a> (Table 9) <li><a href="103063?version=1&table=Table 11">DSIG/DTT_M</a> (Table 11) <li><a href="103063?version=1&table=Table 13">1/SIG*DSIG/DABS_T2_Y</a> (Table 13) <li><a href="103063?version=1&table=Table 15">DSIG/DABS_T2_Y</a> (Table 15) <li><a href="103063?version=1&table=Table 17">1/SIG*DSIG/DABS_TT_Y</a> (Table 17) <li><a href="103063?version=1&table=Table 19">DSIG/DABS_TT_Y</a> (Table 19) <li><a href="103063?version=1&table=Table 21">1/SIG*DSIG/DT1_PT</a> (Table 21) <li><a href="103063?version=1&table=Table 23">DSIG/DT1_PT</a> (Table 23) <li><a href="103063?version=1&table=Table 25">1/SIG*DSIG/DT2_PT</a> (Table 25) <li><a href="103063?version=1&table=Table 27">DSIG/DT2_PT</a> (Table 27) <li><a href="103063?version=1&table=Table 29">1/SIG*DSIG/DTT_PT</a> (Table 29) <li><a href="103063?version=1&table=Table 31">DSIG/DTT_PT</a> (Table 31) <li><a href="103063?version=1&table=Table 33">1/SIG*DSIG/DN_JETS</a> (Table 33) <li><a href="103063?version=1&table=Table 35">DSIG/DN_JETS</a> (Table 35) <li><a href="103063?version=1&table=Table 37">1/SIG*DSIG/DDELTAPHI</a> (Table 37) <li><a href="103063?version=1&table=Table 39">DSIG/DDELTAPHI</a> (Table 39) <li><a href="103063?version=1&table=Table 41">1/SIG*DSIG/DABSPOUT</a> (Table 41) <li><a href="103063?version=1&table=Table 43">DSIG/DABSPOUT</a> (Table 43) <li><a href="103063?version=1&table=Table 45">1/SIG*DSIG/DABSPCROSS</a> (Table 45) <li><a href="103063?version=1&table=Table 47">DSIG/DABSPCROSS</a> (Table 47) <li><a href="103063?version=1&table=Table 49">1/SIG*DSIG/DZ_TT</a> (Table 49) <li><a href="103063?version=1&table=Table 51">DSIG/DZ_TT</a> (Table 51) <li><a href="103063?version=1&table=Table 53">1/SIG*DSIG/DHT_TT</a> (Table 53) <li><a href="103063?version=1&table=Table 55">DSIG/DHT_TT</a> (Table 55) <li><a href="103063?version=1&table=Table 57">1/SIG*DSIG/DABS_Y_BOOST </a> (Table 57) <li><a href="103063?version=1&table=Table 59">DSIG/DABS_Y_BOOST </a> (Table 59) <li><a href="103063?version=1&table=Table 61">1/SIG*DSIG/DCHI_TT</a> (Table 61) <li><a href="103063?version=1&table=Table 63">DSIG/DCHI_TT</a> (Table 63) <li><a href="103063?version=1&table=Table 65">1/SIG*DSIG/DRWT1</a> (Table 65) <li><a href="103063?version=1&table=Table 67">DSIG/DRWT1</a> (Table 67) <li><a href="103063?version=1&table=Table 69">1/SIG*DSIG/DRWT2</a> (Table 69) <li><a href="103063?version=1&table=Table 71">DSIG/DRWT2</a> (Table 71) <li><a href="103063?version=1&table=Table 73">1/SIG*DSIG/DRWB1</a> (Table 73) <li><a href="103063?version=1&table=Table 75">DSIG/DRWB1</a> (Table 75) <li><a href="103063?version=1&table=Table 77">1/SIG*DSIG/DRWB2</a> (Table 77) <li><a href="103063?version=1&table=Table 79">DSIG/DRWB2</a> (Table 79) <li><a href="103063?version=1&table=Table 81">1/SIG*DSIG/DDR_E1TC</a> (Table 81) <li><a href="103063?version=1&table=Table 83">DSIG/DDR_E1TC</a> (Table 83) <li><a href="103063?version=1&table=Table 85">1/SIG*DSIG/DDR_E2TC</a> (Table 85) <li><a href="103063?version=1&table=Table 87">DSIG/DDR_E2TC</a> (Table 87) <li><a href="103063?version=1&table=Table 89">1/SIG*DSIG/DDR_E3TC</a> (Table 89) <li><a href="103063?version=1&table=Table 91">DSIG/DDR_E3TC</a> (Table 91) <li><a href="103063?version=1&table=Table 93">1/SIG*DSIG/DRPT_E1T1</a> (Table 93) <li><a href="103063?version=1&table=Table 95">DSIG/DRPT_E1T1</a> (Table 95) <li><a href="103063?version=1&table=Table 97">1/SIG*DSIG/DRPT_E2T1</a> (Table 97) <li><a href="103063?version=1&table=Table 99">DSIG/DRPT_E2T1</a> (Table 99) <li><a href="103063?version=1&table=Table 101">1/SIG*DSIG/DRPT_E3T1</a> (Table 101) <li><a href="103063?version=1&table=Table 103">DSIG/DRPT_E3T1</a> (Table 103) <li><a href="103063?version=1&table=Table 105">1/SIG*DSIG/DRPT_TTE1</a> (Table 105) <li><a href="103063?version=1&table=Table 107">DSIG/DRPT_TTE1</a> (Table 107) <li><a href="103063?version=1&table=Table 109">1/SIG*DSIG/DRPT_E1J1</a> (Table 109) <li><a href="103063?version=1&table=Table 111">DSIG/DRPT_E1J1</a> (Table 111) <li><a href="103063?version=1&table=Table 113">1/SIG*DSIG/DRPT_E2J1</a> (Table 113) <li><a href="103063?version=1&table=Table 115">DSIG/DRPT_E2J1</a> (Table 115) <li><a href="103063?version=1&table=Table 117">1/SIG*DSIG/DRPT_E3J1</a> (Table 117) <li><a href="103063?version=1&table=Table 119">DSIG/DRPT_E3J1</a> (Table 119) <li><a href="103063?version=1&table=Table 121">1/SIG*DSIG/DDR_E2E1</a> (Table 121) <li><a href="103063?version=1&table=Table 123">DSIG/DDR_E2E1</a> (Table 123) <li><a href="103063?version=1&table=Table 125">1/SIG*DSIG/DDR_E3E1</a> (Table 125) <li><a href="103063?version=1&table=Table 127">DSIG/DDR_E3E1</a> (Table 127) <li><a href="103063?version=1&table=Table 129">1/SIG*DSIG/DRPT_E2E1</a> (Table 129) <li><a href="103063?version=1&table=Table 131">DSIG/DRPT_E2E1</a> (Table 131) <li><a href="103063?version=1&table=Table 133">1/SIG*DSIG/DRPT_E3E1</a> (Table 133) <li><a href="103063?version=1&table=Table 135">DSIG/DRPT_E3E1</a> (Table 135) <li><a href="103063?version=1&table=Table 137">SIG</a> (Table 137) </ul><br/> Covariances: <ul> <li><a href="103063?version=1&table=Table 2">1/SIG*DSIG/DDR_E1J1</a> (Table 2) <li><a href="103063?version=1&table=Table 4">DSIG/DDR_E1J1</a> (Table 4) <li><a href="103063?version=1&table=Table 6">1/SIG*DSIG/DABS_T1_Y</a> (Table 6) <li><a href="103063?version=1&table=Table 8">DSIG/DABS_T1_Y</a> (Table 8) <li><a href="103063?version=1&table=Table 10">1/SIG*DSIG/DTT_M</a> (Table 10) <li><a href="103063?version=1&table=Table 12">DSIG/DTT_M</a> (Table 12) <li><a href="103063?version=1&table=Table 14">1/SIG*DSIG/DABS_T2_Y</a> (Table 14) <li><a href="103063?version=1&table=Table 16">DSIG/DABS_T2_Y</a> (Table 16) <li><a href="103063?version=1&table=Table 18">1/SIG*DSIG/DABS_TT_Y</a> (Table 18) <li><a href="103063?version=1&table=Table 20">DSIG/DABS_TT_Y</a> (Table 20) <li><a href="103063?version=1&table=Table 22">1/SIG*DSIG/DT1_PT</a> (Table 22) <li><a href="103063?version=1&table=Table 24">DSIG/DT1_PT</a> (Table 24) <li><a href="103063?version=1&table=Table 26">1/SIG*DSIG/DT2_PT</a> (Table 26) <li><a href="103063?version=1&table=Table 28">DSIG/DT2_PT</a> (Table 28) <li><a href="103063?version=1&table=Table 30">1/SIG*DSIG/DTT_PT</a> (Table 30) <li><a href="103063?version=1&table=Table 32">DSIG/DTT_PT</a> (Table 32) <li><a href="103063?version=1&table=Table 34">1/SIG*DSIG/DN_JETS</a> (Table 34) <li><a href="103063?version=1&table=Table 36">DSIG/DN_JETS</a> (Table 36) <li><a href="103063?version=1&table=Table 38">1/SIG*DSIG/DDELTAPHI</a> (Table 38) <li><a href="103063?version=1&table=Table 40">DSIG/DDELTAPHI</a> (Table 40) <li><a href="103063?version=1&table=Table 42">1/SIG*DSIG/DABSPOUT</a> (Table 42) <li><a href="103063?version=1&table=Table 44">DSIG/DABSPOUT</a> (Table 44) <li><a href="103063?version=1&table=Table 46">1/SIG*DSIG/DABSPCROSS</a> (Table 46) <li><a href="103063?version=1&table=Table 48">DSIG/DABSPCROSS</a> (Table 48) <li><a href="103063?version=1&table=Table 50">1/SIG*DSIG/DZ_TT</a> (Table 50) <li><a href="103063?version=1&table=Table 52">DSIG/DZ_TT</a> (Table 52) <li><a href="103063?version=1&table=Table 54">1/SIG*DSIG/DHT_TT</a> (Table 54) <li><a href="103063?version=1&table=Table 56">DSIG/DHT_TT</a> (Table 56) <li><a href="103063?version=1&table=Table 58">1/SIG*DSIG/DABS_Y_BOOST </a> (Table 58) <li><a href="103063?version=1&table=Table 60">DSIG/DABS_Y_BOOST </a> (Table 60) <li><a href="103063?version=1&table=Table 62">1/SIG*DSIG/DCHI_TT</a> (Table 62) <li><a href="103063?version=1&table=Table 64">DSIG/DCHI_TT</a> (Table 64) <li><a href="103063?version=1&table=Table 66">1/SIG*DSIG/DRWT1</a> (Table 66) <li><a href="103063?version=1&table=Table 68">DSIG/DRWT1</a> (Table 68) <li><a href="103063?version=1&table=Table 70">1/SIG*DSIG/DRWT2</a> (Table 70) <li><a href="103063?version=1&table=Table 72">DSIG/DRWT2</a> (Table 72) <li><a href="103063?version=1&table=Table 74">1/SIG*DSIG/DRWB1</a> (Table 74) <li><a href="103063?version=1&table=Table 76">DSIG/DRWB1</a> (Table 76) <li><a href="103063?version=1&table=Table 78">1/SIG*DSIG/DRWB2</a> (Table 78) <li><a href="103063?version=1&table=Table 80">DSIG/DRWB2</a> (Table 80) <li><a href="103063?version=1&table=Table 82">1/SIG*DSIG/DDR_E1TC</a> (Table 82) <li><a href="103063?version=1&table=Table 84">DSIG/DDR_E1TC</a> (Table 84) <li><a href="103063?version=1&table=Table 86">1/SIG*DSIG/DDR_E2TC</a> (Table 86) <li><a href="103063?version=1&table=Table 88">DSIG/DDR_E2TC</a> (Table 88) <li><a href="103063?version=1&table=Table 90">1/SIG*DSIG/DDR_E3TC</a> (Table 90) <li><a href="103063?version=1&table=Table 92">DSIG/DDR_E3TC</a> (Table 92) <li><a href="103063?version=1&table=Table 94">1/SIG*DSIG/DRPT_E1T1</a> (Table 94) <li><a href="103063?version=1&table=Table 96">DSIG/DRPT_E1T1</a> (Table 96) <li><a href="103063?version=1&table=Table 98">1/SIG*DSIG/DRPT_E2T1</a> (Table 98) <li><a href="103063?version=1&table=Table 100">DSIG/DRPT_E2T1</a> (Table 100) <li><a href="103063?version=1&table=Table 102">1/SIG*DSIG/DRPT_E3T1</a> (Table 102) <li><a href="103063?version=1&table=Table 104">DSIG/DRPT_E3T1</a> (Table 104) <li><a href="103063?version=1&table=Table 106">1/SIG*DSIG/DRPT_TTE1</a> (Table 106) <li><a href="103063?version=1&table=Table 108">DSIG/DRPT_TTE1</a> (Table 108) <li><a href="103063?version=1&table=Table 110">1/SIG*DSIG/DRPT_E1J1</a> (Table 110) <li><a href="103063?version=1&table=Table 112">DSIG/DRPT_E1J1</a> (Table 112) <li><a href="103063?version=1&table=Table 114">1/SIG*DSIG/DRPT_E2J1</a> (Table 114) <li><a href="103063?version=1&table=Table 116">DSIG/DRPT_E2J1</a> (Table 116) <li><a href="103063?version=1&table=Table 118">1/SIG*DSIG/DRPT_E3J1</a> (Table 118) <li><a href="103063?version=1&table=Table 120">DSIG/DRPT_E3J1</a> (Table 120) <li><a href="103063?version=1&table=Table 122">1/SIG*DSIG/DDR_E2E1</a> (Table 122) <li><a href="103063?version=1&table=Table 124">DSIG/DDR_E2E1</a> (Table 124) <li><a href="103063?version=1&table=Table 126">1/SIG*DSIG/DDR_E3E1</a> (Table 126) <li><a href="103063?version=1&table=Table 128">DSIG/DDR_E3E1</a> (Table 128) <li><a href="103063?version=1&table=Table 130">1/SIG*DSIG/DRPT_E2E1</a> (Table 130) <li><a href="103063?version=1&table=Table 132">DSIG/DRPT_E2E1</a> (Table 132) <li><a href="103063?version=1&table=Table 134">1/SIG*DSIG/DRPT_E3E1</a> (Table 134) <li><a href="103063?version=1&table=Table 136">DSIG/DRPT_E3E1</a> (Table 136) </ul><br/> <u>2D:</u><br/> Spectra: <ul> <li><a href="103063?version=1&table=Table 138">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 6)</a> (Table 138) <li><a href="103063?version=1&table=Table 139">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 7)</a> (Table 139) <li><a href="103063?version=1&table=Table 140">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 8)</a> (Table 140) <li><a href="103063?version=1&table=Table 141">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS > 8)</a> (Table 141) <li><a href="103063?version=1&table=Table 152">D2SIG/DT1_PT/DN_JETS (N_JETS = 6)</a> (Table 152) <li><a href="103063?version=1&table=Table 153">D2SIG/DT1_PT/DN_JETS (N_JETS = 7)</a> (Table 153) <li><a href="103063?version=1&table=Table 154">D2SIG/DT1_PT/DN_JETS (N_JETS = 8)</a> (Table 154) <li><a href="103063?version=1&table=Table 155">D2SIG/DT1_PT/DN_JETS (N_JETS > 8)</a> (Table 155) <li><a href="103063?version=1&table=Table 166">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 6)</a> (Table 166) <li><a href="103063?version=1&table=Table 167">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 7)</a> (Table 167) <li><a href="103063?version=1&table=Table 168">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 8)</a> (Table 168) <li><a href="103063?version=1&table=Table 169">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS > 8)</a> (Table 169) <li><a href="103063?version=1&table=Table 180">D2SIG/DT2_PT/DN_JETS (N_JETS = 6)</a> (Table 180) <li><a href="103063?version=1&table=Table 181">D2SIG/DT2_PT/DN_JETS (N_JETS = 7)</a> (Table 181) <li><a href="103063?version=1&table=Table 182">D2SIG/DT2_PT/DN_JETS (N_JETS = 8)</a> (Table 182) <li><a href="103063?version=1&table=Table 183">D2SIG/DT2_PT/DN_JETS (N_JETS > 8)</a> (Table 183) <li><a href="103063?version=1&table=Table 194">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 6)</a> (Table 194) <li><a href="103063?version=1&table=Table 195">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 7)</a> (Table 195) <li><a href="103063?version=1&table=Table 196">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 8)</a> (Table 196) <li><a href="103063?version=1&table=Table 197">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS > 8)</a> (Table 197) <li><a href="103063?version=1&table=Table 208">D2SIG/DTT_PT/DN_JETS (N_JETS = 6)</a> (Table 208) <li><a href="103063?version=1&table=Table 209">D2SIG/DTT_PT/DN_JETS (N_JETS = 7)</a> (Table 209) <li><a href="103063?version=1&table=Table 210">D2SIG/DTT_PT/DN_JETS (N_JETS = 8)</a> (Table 210) <li><a href="103063?version=1&table=Table 211">D2SIG/DTT_PT/DN_JETS (N_JETS > 8)</a> (Table 211) <li><a href="103063?version=1&table=Table 222">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 6)</a> (Table 222) <li><a href="103063?version=1&table=Table 223">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 7)</a> (Table 223) <li><a href="103063?version=1&table=Table 224">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 8)</a> (Table 224) <li><a href="103063?version=1&table=Table 225">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS > 8)</a> (Table 225) <li><a href="103063?version=1&table=Table 236">D2SIG/DABSPOUT/DN_JETS (N_JETS = 6)</a> (Table 236) <li><a href="103063?version=1&table=Table 237">D2SIG/DABSPOUT/DN_JETS (N_JETS = 7)</a> (Table 237) <li><a href="103063?version=1&table=Table 238">D2SIG/DABSPOUT/DN_JETS (N_JETS = 8)</a> (Table 238) <li><a href="103063?version=1&table=Table 239">D2SIG/DABSPOUT/DN_JETS (N_JETS > 8)</a> (Table 239) <li><a href="103063?version=1&table=Table 250">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 6)</a> (Table 250) <li><a href="103063?version=1&table=Table 251">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 7)</a> (Table 251) <li><a href="103063?version=1&table=Table 252">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 8)</a> (Table 252) <li><a href="103063?version=1&table=Table 253">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS > 8)</a> (Table 253) <li><a href="103063?version=1&table=Table 264">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 6)</a> (Table 264) <li><a href="103063?version=1&table=Table 265">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 7)</a> (Table 265) <li><a href="103063?version=1&table=Table 266">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 8)</a> (Table 266) <li><a href="103063?version=1&table=Table 267">D2SIG/DDELTAPHI/DN_JETS (N_JETS > 8)</a> (Table 267) <li><a href="103063?version=1&table=Table 278">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 6)</a> (Table 278) <li><a href="103063?version=1&table=Table 279">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 7)</a> (Table 279) <li><a href="103063?version=1&table=Table 280">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 8)</a> (Table 280) <li><a href="103063?version=1&table=Table 281">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS > 8)</a> (Table 281) <li><a href="103063?version=1&table=Table 292">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 6)</a> (Table 292) <li><a href="103063?version=1&table=Table 293">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 7)</a> (Table 293) <li><a href="103063?version=1&table=Table 294">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 8)</a> (Table 294) <li><a href="103063?version=1&table=Table 295">D2SIG/DABSPCROSS/DN_JETS (N_JETS > 8)</a> (Table 295) <li><a href="103063?version=1&table=Table 306">1/SIG*D2SIG/DT2_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 306) <li><a href="103063?version=1&table=Table 307">1/SIG*D2SIG/DT2_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 307) <li><a href="103063?version=1&table=Table 308">1/SIG*D2SIG/DT2_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 308) <li><a href="103063?version=1&table=Table 309">1/SIG*D2SIG/DT2_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 309) <li><a href="103063?version=1&table=Table 320">D2SIG/DT2_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 320) <li><a href="103063?version=1&table=Table 321">D2SIG/DT2_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 321) <li><a href="103063?version=1&table=Table 322">D2SIG/DT2_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 322) <li><a href="103063?version=1&table=Table 323">D2SIG/DT2_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 323) <li><a href="103063?version=1&table=Table 334">1/SIG*D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 334) <li><a href="103063?version=1&table=Table 335">1/SIG*D2SIG/DTT_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 335) <li><a href="103063?version=1&table=Table 336">1/SIG*D2SIG/DTT_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 336) <li><a href="103063?version=1&table=Table 337">1/SIG*D2SIG/DTT_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 337) <li><a href="103063?version=1&table=Table 348">D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 348) <li><a href="103063?version=1&table=Table 349">D2SIG/DTT_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 349) <li><a href="103063?version=1&table=Table 350">D2SIG/DTT_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 350) <li><a href="103063?version=1&table=Table 351">D2SIG/DTT_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 351) <li><a href="103063?version=1&table=Table 362">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 362) <li><a href="103063?version=1&table=Table 363">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 363) <li><a href="103063?version=1&table=Table 364">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 364) <li><a href="103063?version=1&table=Table 365">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 365) <li><a href="103063?version=1&table=Table 376">D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 376) <li><a href="103063?version=1&table=Table 377">D2SIG/DABS_TT_Y/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 377) <li><a href="103063?version=1&table=Table 378">D2SIG/DABS_TT_Y/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 378) <li><a href="103063?version=1&table=Table 379">D2SIG/DABS_TT_Y/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 379) <li><a href="103063?version=1&table=Table 390">1/SIG*D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 175.0 GeV)</a> (Table 390) <li><a href="103063?version=1&table=Table 391">1/SIG*D2SIG/DT1_PT/DT2_PT ( 175.0 GeV < T2_PT < 275.0 GeV)</a> (Table 391) <li><a href="103063?version=1&table=Table 392">1/SIG*D2SIG/DT1_PT/DT2_PT ( 275.0 GeV < T2_PT < 385.0 GeV)</a> (Table 392) <li><a href="103063?version=1&table=Table 393">1/SIG*D2SIG/DT1_PT/DT2_PT ( 385.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 393) <li><a href="103063?version=1&table=Table 404">D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 175.0 GeV)</a> (Table 404) <li><a href="103063?version=1&table=Table 405">D2SIG/DT1_PT/DT2_PT ( 175.0 GeV < T2_PT < 275.0 GeV)</a> (Table 405) <li><a href="103063?version=1&table=Table 406">D2SIG/DT1_PT/DT2_PT ( 275.0 GeV < T2_PT < 385.0 GeV)</a> (Table 406) <li><a href="103063?version=1&table=Table 407">D2SIG/DT1_PT/DT2_PT ( 385.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 407) <li><a href="103063?version=1&table=Table 418">1/SIG*D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 645.0 GeV)</a> (Table 418) <li><a href="103063?version=1&table=Table 419">1/SIG*D2SIG/DT1_PT/DTT_M ( 645.0 GeV < TT_M < 795.0 GeV)</a> (Table 419) <li><a href="103063?version=1&table=Table 420">1/SIG*D2SIG/DT1_PT/DTT_M ( 795.0 GeV < TT_M < 1080.0 GeV)</a> (Table 420) <li><a href="103063?version=1&table=Table 421">1/SIG*D2SIG/DT1_PT/DTT_M ( 1080.0 GeV < TT_M < 3000.0 GeV)</a> (Table 421) <li><a href="103063?version=1&table=Table 432">D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 645.0 GeV)</a> (Table 432) <li><a href="103063?version=1&table=Table 433">D2SIG/DT1_PT/DTT_M ( 645.0 GeV < TT_M < 795.0 GeV)</a> (Table 433) <li><a href="103063?version=1&table=Table 434">D2SIG/DT1_PT/DTT_M ( 795.0 GeV < TT_M < 1080.0 GeV)</a> (Table 434) <li><a href="103063?version=1&table=Table 435">D2SIG/DT1_PT/DTT_M ( 1080.0 GeV < TT_M < 3000.0 GeV)</a> (Table 435) </ul><br/> Covariances:<br/><ul> <li><a href="103063?version=1&table=Table 142">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 142) <li><a href="103063?version=1&table=Table 143">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 143) <li><a href="103063?version=1&table=Table 144">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 144) <li><a href="103063?version=1&table=Table 145">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 145) <li><a href="103063?version=1&table=Table 146">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 146) <li><a href="103063?version=1&table=Table 147">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 147) <li><a href="103063?version=1&table=Table 148">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 148) <li><a href="103063?version=1&table=Table 149">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 149) <li><a href="103063?version=1&table=Table 150">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 150) <li><a href="103063?version=1&table=Table 151">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 151) <li><a href="103063?version=1&table=Table 156">Matrix for D2SIG/DT1_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 156) <li><a href="103063?version=1&table=Table 157">Matrix for D2SIG/DT1_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 157) <li><a href="103063?version=1&table=Table 158">Matrix for D2SIG/DT1_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 158) <li><a href="103063?version=1&table=Table 159">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 159) <li><a href="103063?version=1&table=Table 160">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 160) <li><a href="103063?version=1&table=Table 161">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 161) <li><a href="103063?version=1&table=Table 162">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 162) <li><a href="103063?version=1&table=Table 163">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 163) <li><a href="103063?version=1&table=Table 164">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 164) <li><a href="103063?version=1&table=Table 165">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 165) <li><a href="103063?version=1&table=Table 170">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 170) <li><a href="103063?version=1&table=Table 171">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 171) <li><a href="103063?version=1&table=Table 172">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 172) <li><a href="103063?version=1&table=Table 173">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 173) <li><a href="103063?version=1&table=Table 174">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 174) <li><a href="103063?version=1&table=Table 175">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 175) <li><a href="103063?version=1&table=Table 176">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 176) <li><a href="103063?version=1&table=Table 177">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 177) <li><a href="103063?version=1&table=Table 178">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 178) <li><a href="103063?version=1&table=Table 179">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 179) <li><a href="103063?version=1&table=Table 184">Matrix for D2SIG/DT2_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 184) <li><a href="103063?version=1&table=Table 185">Matrix for D2SIG/DT2_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 185) <li><a href="103063?version=1&table=Table 186">Matrix for D2SIG/DT2_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 186) <li><a href="103063?version=1&table=Table 187">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 187) <li><a href="103063?version=1&table=Table 188">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 188) <li><a href="103063?version=1&table=Table 189">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 189) <li><a href="103063?version=1&table=Table 190">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 190) <li><a href="103063?version=1&table=Table 191">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 191) <li><a href="103063?version=1&table=Table 192">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 192) <li><a href="103063?version=1&table=Table 193">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 193) <li><a href="103063?version=1&table=Table 198">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 198) <li><a href="103063?version=1&table=Table 199">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 199) <li><a href="103063?version=1&table=Table 200">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 200) <li><a href="103063?version=1&table=Table 201">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 201) <li><a href="103063?version=1&table=Table 202">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 202) <li><a href="103063?version=1&table=Table 203">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 203) <li><a href="103063?version=1&table=Table 204">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 204) <li><a href="103063?version=1&table=Table 205">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 205) <li><a href="103063?version=1&table=Table 206">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 206) <li><a href="103063?version=1&table=Table 207">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 207) <li><a href="103063?version=1&table=Table 212">Matrix for D2SIG/DTT_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 212) <li><a href="103063?version=1&table=Table 213">Matrix for D2SIG/DTT_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 213) <li><a href="103063?version=1&table=Table 214">Matrix for D2SIG/DTT_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 214) <li><a href="103063?version=1&table=Table 215">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 215) <li><a href="103063?version=1&table=Table 216">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 216) <li><a href="103063?version=1&table=Table 217">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 217) <li><a href="103063?version=1&table=Table 218">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 218) <li><a href="103063?version=1&table=Table 219">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 219) <li><a href="103063?version=1&table=Table 220">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 220) <li><a href="103063?version=1&table=Table 221">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 221) <li><a href="103063?version=1&table=Table 226">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 226) <li><a href="103063?version=1&table=Table 227">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 227) <li><a href="103063?version=1&table=Table 228">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 228) <li><a href="103063?version=1&table=Table 229">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 229) <li><a href="103063?version=1&table=Table 230">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 230) <li><a href="103063?version=1&table=Table 231">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 231) <li><a href="103063?version=1&table=Table 232">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 232) <li><a href="103063?version=1&table=Table 233">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 233) <li><a href="103063?version=1&table=Table 234">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 234) <li><a href="103063?version=1&table=Table 235">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 235) <li><a href="103063?version=1&table=Table 240">Matrix for D2SIG/DABSPOUT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 240) <li><a href="103063?version=1&table=Table 241">Matrix for D2SIG/DABSPOUT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 241) <li><a href="103063?version=1&table=Table 242">Matrix for D2SIG/DABSPOUT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 242) <li><a href="103063?version=1&table=Table 243">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 243) <li><a href="103063?version=1&table=Table 244">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 244) <li><a href="103063?version=1&table=Table 245">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 245) <li><a href="103063?version=1&table=Table 246">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 246) <li><a href="103063?version=1&table=Table 247">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 247) <li><a href="103063?version=1&table=Table 248">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 248) <li><a href="103063?version=1&table=Table 249">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 249) <li><a href="103063?version=1&table=Table 254">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 254) <li><a href="103063?version=1&table=Table 255">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 255) <li><a href="103063?version=1&table=Table 256">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 256) <li><a href="103063?version=1&table=Table 257">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 257) <li><a href="103063?version=1&table=Table 258">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 258) <li><a href="103063?version=1&table=Table 259">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 259) <li><a href="103063?version=1&table=Table 260">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 260) <li><a href="103063?version=1&table=Table 261">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 261) <li><a href="103063?version=1&table=Table 262">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 262) <li><a href="103063?version=1&table=Table 263">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 263) <li><a href="103063?version=1&table=Table 268">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 268) <li><a href="103063?version=1&table=Table 269">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 269) <li><a href="103063?version=1&table=Table 270">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 270) <li><a href="103063?version=1&table=Table 271">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 271) <li><a href="103063?version=1&table=Table 272">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 272) <li><a href="103063?version=1&table=Table 273">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 273) <li><a href="103063?version=1&table=Table 274">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 274) <li><a href="103063?version=1&table=Table 275">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 275) <li><a href="103063?version=1&table=Table 276">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 276) <li><a href="103063?version=1&table=Table 277">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 277) <li><a href="103063?version=1&table=Table 282">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 282) <li><a href="103063?version=1&table=Table 283">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 283) <li><a href="103063?version=1&table=Table 284">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 284) <li><a href="103063?version=1&table=Table 285">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 285) <li><a href="103063?version=1&table=Table 286">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 286) <li><a href="103063?version=1&table=Table 287">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 287) <li><a href="103063?version=1&table=Table 288">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 288) <li><a href="103063?version=1&table=Table 289">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 289) <li><a href="103063?version=1&table=Table 290">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 290) <li><a href="103063?version=1&table=Table 291">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 291) <li><a href="103063?version=1&table=Table 296">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 296) <li><a href="103063?version=1&table=Table 297">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 297) <li><a href="103063?version=1&table=Table 298">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 298) <li><a href="103063?version=1&table=Table 299">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 299) <li><a href="103063?version=1&table=Table 300">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 300) <li><a href="103063?version=1&table=Table 301">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 301) <li><a href="103063?version=1&table=Table 302">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 302) <li><a href="103063?version=1&table=Table 303">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 303) <li><a href="103063?version=1&table=Table 304">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 304) <li><a href="103063?version=1&table=Table 305">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 305) <li><a href="103063?version=1&table=Table 310">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 310) <li><a href="103063?version=1&table=Table 311">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 311) <li><a href="103063?version=1&table=Table 312">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 312) <li><a href="103063?version=1&table=Table 313">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 313) <li><a href="103063?version=1&table=Table 314">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 314) <li><a href="103063?version=1&table=Table 315">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 315) <li><a href="103063?version=1&table=Table 316">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 316) <li><a href="103063?version=1&table=Table 317">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 317) <li><a href="103063?version=1&table=Table 318">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 318) <li><a href="103063?version=1&table=Table 319">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 319) <li><a href="103063?version=1&table=Table 324">Matrix for D2SIG/DT2_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 324) <li><a href="103063?version=1&table=Table 325">Matrix for D2SIG/DT2_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 325) <li><a href="103063?version=1&table=Table 326">Matrix for D2SIG/DT2_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 326) <li><a href="103063?version=1&table=Table 327">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 327) <li><a href="103063?version=1&table=Table 328">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 328) <li><a href="103063?version=1&table=Table 329">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 329) <li><a href="103063?version=1&table=Table 330">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 330) <li><a href="103063?version=1&table=Table 331">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 331) <li><a href="103063?version=1&table=Table 332">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 332) <li><a href="103063?version=1&table=Table 333">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 333) <li><a href="103063?version=1&table=Table 338">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 338) <li><a href="103063?version=1&table=Table 339">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 339) <li><a href="103063?version=1&table=Table 340">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 340) <li><a href="103063?version=1&table=Table 341">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 341) <li><a href="103063?version=1&table=Table 342">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 342) <li><a href="103063?version=1&table=Table 343">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 343) <li><a href="103063?version=1&table=Table 344">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 344) <li><a href="103063?version=1&table=Table 345">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 345) <li><a href="103063?version=1&table=Table 346">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 346) <li><a href="103063?version=1&table=Table 347">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 347) <li><a href="103063?version=1&table=Table 352">Matrix for D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 352) <li><a href="103063?version=1&table=Table 353">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 353) <li><a href="103063?version=1&table=Table 354">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 354) <li><a href="103063?version=1&table=Table 355">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 355) <li><a href="103063?version=1&table=Table 356">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 356) <li><a href="103063?version=1&table=Table 357">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 357) <li><a href="103063?version=1&table=Table 358">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 358) <li><a href="103063?version=1&table=Table 359">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 359) <li><a href="103063?version=1&table=Table 360">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 360) <li><a href="103063?version=1&table=Table 361">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 361) <li><a href="103063?version=1&table=Table 366">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 366) <li><a href="103063?version=1&table=Table 367">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 367) <li><a href="103063?version=1&table=Table 368">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 368) <li><a href="103063?version=1&table=Table 369">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 369) <li><a href="103063?version=1&table=Table 370">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 370) <li><a href="103063?version=1&table=Table 371">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 371) <li><a href="103063?version=1&table=Table 372">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 1th bins of TT_M</a> (Table 372) <li><a href="103063?version=1&table=Table 373">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 2th bins of TT_M</a> (Table 373) <li><a href="103063?version=1&table=Table 374">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 3th bins of TT_M</a> (Table 374) <li><a href="103063?version=1&table=Table 375">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 4th bins of TT_M</a> (Table 375) <li><a href="103063?version=1&table=Table 380">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 380) <li><a href="103063?version=1&table=Table 381">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 381) <li><a href="103063?version=1&table=Table 382">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 382) <li><a href="103063?version=1&table=Table 383">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 383) <li><a href="103063?version=1&table=Table 384">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 384) <li><a href="103063?version=1&table=Table 385">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 385) <li><a href="103063?version=1&table=Table 386">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 1th bins of TT_M</a> (Table 386) <li><a href="103063?version=1&table=Table 387">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 2th bins of TT_M</a> (Table 387) <li><a href="103063?version=1&table=Table 388">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 3th bins of TT_M</a> (Table 388) <li><a href="103063?version=1&table=Table 389">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 4th bins of TT_M</a> (Table 389) <li><a href="103063?version=1&table=Table 394">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 394) <li><a href="103063?version=1&table=Table 395">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 395) <li><a href="103063?version=1&table=Table 396">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 396) <li><a href="103063?version=1&table=Table 397">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 397) <li><a href="103063?version=1&table=Table 398">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 398) <li><a href="103063?version=1&table=Table 399">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 399) <li><a href="103063?version=1&table=Table 400">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 400) <li><a href="103063?version=1&table=Table 401">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 401) <li><a href="103063?version=1&table=Table 402">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 402) <li><a href="103063?version=1&table=Table 403">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 403) <li><a href="103063?version=1&table=Table 408">Matrix for D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 408) <li><a href="103063?version=1&table=Table 409">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 409) <li><a href="103063?version=1&table=Table 410">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 410) <li><a href="103063?version=1&table=Table 411">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 411) <li><a href="103063?version=1&table=Table 412">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 412) <li><a href="103063?version=1&table=Table 413">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 413) <li><a href="103063?version=1&table=Table 414">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 414) <li><a href="103063?version=1&table=Table 415">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 415) <li><a href="103063?version=1&table=Table 416">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 416) <li><a href="103063?version=1&table=Table 417">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 417) <li><a href="103063?version=1&table=Table 422">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 422) <li><a href="103063?version=1&table=Table 423">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 423) <li><a href="103063?version=1&table=Table 424">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 424) <li><a href="103063?version=1&table=Table 425">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 425) <li><a href="103063?version=1&table=Table 426">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 426) <li><a href="103063?version=1&table=Table 427">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 427) <li><a href="103063?version=1&table=Table 428">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 428) <li><a href="103063?version=1&table=Table 429">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 429) <li><a href="103063?version=1&table=Table 430">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 430) <li><a href="103063?version=1&table=Table 431">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 431) <li><a href="103063?version=1&table=Table 436">Matrix for D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 436) <li><a href="103063?version=1&table=Table 437">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 437) <li><a href="103063?version=1&table=Table 438">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 438) <li><a href="103063?version=1&table=Table 439">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 439) <li><a href="103063?version=1&table=Table 440">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 440) <li><a href="103063?version=1&table=Table 441">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 441) <li><a href="103063?version=1&table=Table 442">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 442) <li><a href="103063?version=1&table=Table 443">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 443) <li><a href="103063?version=1&table=Table 444">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 444) <li><a href="103063?version=1&table=Table 445">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 445) </ul><br/> <b>Parton level:</b><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 446">1/SIG*DSIG/DCHI_TT</a> (Table 446) <li><a href="103063?version=1&table=Table 448">DSIG/DCHI_TT</a> (Table 448) <li><a href="103063?version=1&table=Table 450">1/SIG*DSIG/DTT_PT</a> (Table 450) <li><a href="103063?version=1&table=Table 452">DSIG/DTT_PT</a> (Table 452) <li><a href="103063?version=1&table=Table 454">1/SIG*DSIG/DDELTAPHI</a> (Table 454) <li><a href="103063?version=1&table=Table 456">DSIG/DDELTAPHI</a> (Table 456) <li><a href="103063?version=1&table=Table 458">1/SIG*DSIG/DT2_PT</a> (Table 458) <li><a href="103063?version=1&table=Table 460">DSIG/DT2_PT</a> (Table 460) <li><a href="103063?version=1&table=Table 462">1/SIG*DSIG/DTT_M</a> (Table 462) <li><a href="103063?version=1&table=Table 464">DSIG/DTT_M</a> (Table 464) <li><a href="103063?version=1&table=Table 466">1/SIG*DSIG/DABS_Y_BOOST</a> (Table 466) <li><a href="103063?version=1&table=Table 468">DSIG/DABS_Y_BOOST</a> (Table 468) <li><a href="103063?version=1&table=Table 470">1/SIG*DSIG/DT1_PT</a> (Table 470) <li><a href="103063?version=1&table=Table 472">DSIG/DT1_PT</a> (Table 472) <li><a href="103063?version=1&table=Table 474">1/SIG*DSIG/DABS_TT_Y</a> (Table 474) <li><a href="103063?version=1&table=Table 476">DSIG/DABS_TT_Y</a> (Table 476) <li><a href="103063?version=1&table=Table 478">1/SIG*DSIG/DABS_T2_Y</a> (Table 478) <li><a href="103063?version=1&table=Table 480">DSIG/DABS_T2_Y</a> (Table 480) <li><a href="103063?version=1&table=Table 482">1/SIG*DSIG/DHT_TT</a> (Table 482) <li><a href="103063?version=1&table=Table 484">DSIG/DHT_TT</a> (Table 484) <li><a href="103063?version=1&table=Table 486">1/SIG*DSIG/DABS_T1_Y</a> (Table 486) <li><a href="103063?version=1&table=Table 488">DSIG/DABS_T1_Y</a> (Table 488) </ul><br/> Covariances:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 447">1/SIG*DSIG/DCHI_TT</a> (Table 447) <li><a href="103063?version=1&table=Table 449">DSIG/DCHI_TT</a> (Table 449) <li><a href="103063?version=1&table=Table 451">1/SIG*DSIG/DTT_PT</a> (Table 451) <li><a href="103063?version=1&table=Table 453">DSIG/DTT_PT</a> (Table 453) <li><a href="103063?version=1&table=Table 455">1/SIG*DSIG/DDELTAPHI</a> (Table 455) <li><a href="103063?version=1&table=Table 457">DSIG/DDELTAPHI</a> (Table 457) <li><a href="103063?version=1&table=Table 459">1/SIG*DSIG/DT2_PT</a> (Table 459) <li><a href="103063?version=1&table=Table 461">DSIG/DT2_PT</a> (Table 461) <li><a href="103063?version=1&table=Table 463">1/SIG*DSIG/DTT_M</a> (Table 463) <li><a href="103063?version=1&table=Table 465">DSIG/DTT_M</a> (Table 465) <li><a href="103063?version=1&table=Table 467">1/SIG*DSIG/DABS_Y_BOOST</a> (Table 467) <li><a href="103063?version=1&table=Table 469">DSIG/DABS_Y_BOOST</a> (Table 469) <li><a href="103063?version=1&table=Table 471">1/SIG*DSIG/DT1_PT</a> (Table 471) <li><a href="103063?version=1&table=Table 473">DSIG/DT1_PT</a> (Table 473) <li><a href="103063?version=1&table=Table 475">1/SIG*DSIG/DABS_TT_Y</a> (Table 475) <li><a href="103063?version=1&table=Table 477">DSIG/DABS_TT_Y</a> (Table 477) <li><a href="103063?version=1&table=Table 479">1/SIG*DSIG/DABS_T2_Y</a> (Table 479) <li><a href="103063?version=1&table=Table 481">DSIG/DABS_T2_Y</a> (Table 481) <li><a href="103063?version=1&table=Table 483">1/SIG*DSIG/DHT_TT</a> (Table 483) <li><a href="103063?version=1&table=Table 485">DSIG/DHT_TT</a> (Table 485) <li><a href="103063?version=1&table=Table 487">1/SIG*DSIG/DABS_T1_Y</a> (Table 487) <li><a href="103063?version=1&table=Table 489">DSIG/DABS_T1_Y</a> (Table 489) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 490">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 490) <li><a href="103063?version=1&table=Table 491">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 491) <li><a href="103063?version=1&table=Table 492">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 492) <li><a href="103063?version=1&table=Table 499">D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 499) <li><a href="103063?version=1&table=Table 500">D2SIG/DABS_TT_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 500) <li><a href="103063?version=1&table=Table 501">D2SIG/DABS_TT_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 501) <li><a href="103063?version=1&table=Table 508">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.0 < ABS_T1_Y < 0.5 )</a> (Table 508) <li><a href="103063?version=1&table=Table 509">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.5 < ABS_T1_Y < 1.0 )</a> (Table 509) <li><a href="103063?version=1&table=Table 510">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.0 < ABS_T1_Y < 1.5 )</a> (Table 510) <li><a href="103063?version=1&table=Table 511">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.5 < ABS_T1_Y < 2.5 )</a> (Table 511) <li><a href="103063?version=1&table=Table 522">D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.0 < ABS_T1_Y < 0.5 )</a> (Table 522) <li><a href="103063?version=1&table=Table 523">D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.5 < ABS_T1_Y < 1.0 )</a> (Table 523) <li><a href="103063?version=1&table=Table 524">D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.0 < ABS_T1_Y < 1.5 )</a> (Table 524) <li><a href="103063?version=1&table=Table 525">D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.5 < ABS_T1_Y < 2.5 )</a> (Table 525) <li><a href="103063?version=1&table=Table 536">1/SIG*D2SIG/DT2_PT/DM ( 0.0 GeV < M < 700.0 GeV)</a> (Table 536) <li><a href="103063?version=1&table=Table 537">1/SIG*D2SIG/DT2_PT/DM ( 700.0 GeV < M < 970.0 GeV)</a> (Table 537) <li><a href="103063?version=1&table=Table 538">1/SIG*D2SIG/DT2_PT/DM ( 970.0 GeV < M < 1315.0 GeV)</a> (Table 538) <li><a href="103063?version=1&table=Table 539">1/SIG*D2SIG/DT2_PT/DM ( 1315.0 GeV < M < 3000.0 GeV)</a> (Table 539) <li><a href="103063?version=1&table=Table 550">D2SIG/DT2_PT/DM ( 0.0 GeV < M < 700.0 GeV)</a> (Table 550) <li><a href="103063?version=1&table=Table 551">D2SIG/DT2_PT/DM ( 700.0 GeV < M < 970.0 GeV)</a> (Table 551) <li><a href="103063?version=1&table=Table 552">D2SIG/DT2_PT/DM ( 970.0 GeV < M < 1315.0 GeV)</a> (Table 552) <li><a href="103063?version=1&table=Table 553">D2SIG/DT2_PT/DM ( 1315.0 GeV < M < 3000.0 GeV)</a> (Table 553) <li><a href="103063?version=1&table=Table 564">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 564) <li><a href="103063?version=1&table=Table 565">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 565) <li><a href="103063?version=1&table=Table 566">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 566) <li><a href="103063?version=1&table=Table 573">D2SIG/DABS_T1_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 573) <li><a href="103063?version=1&table=Table 574">D2SIG/DABS_T1_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 574) <li><a href="103063?version=1&table=Table 575">D2SIG/DABS_T1_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 575) <li><a href="103063?version=1&table=Table 582">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 582) <li><a href="103063?version=1&table=Table 583">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 583) <li><a href="103063?version=1&table=Table 584">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 584) <li><a href="103063?version=1&table=Table 591">D2SIG/DABS_T2_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 591) <li><a href="103063?version=1&table=Table 592">D2SIG/DABS_T2_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 592) <li><a href="103063?version=1&table=Table 593">D2SIG/DABS_T2_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 593) <li><a href="103063?version=1&table=Table 600">1/SIG*D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 600) <li><a href="103063?version=1&table=Table 601">1/SIG*D2SIG/DTT_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 601) <li><a href="103063?version=1&table=Table 602">1/SIG*D2SIG/DTT_PT/DTT_M ( 970.0 GeV < TT_M < 1315.0 GeV)</a> (Table 602) <li><a href="103063?version=1&table=Table 603">1/SIG*D2SIG/DTT_PT/DTT_M ( 1315.0 GeV < TT_M < 3000.0 GeV)</a> (Table 603) <li><a href="103063?version=1&table=Table 614">D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 614) <li><a href="103063?version=1&table=Table 615">D2SIG/DTT_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 615) <li><a href="103063?version=1&table=Table 616">D2SIG/DTT_PT/DTT_M ( 970.0 GeV < TT_M < 1315.0 GeV)</a> (Table 616) <li><a href="103063?version=1&table=Table 617">D2SIG/DTT_PT/DTT_M ( 1315.0 GeV < TT_M < 3000.0 GeV)</a> (Table 617) <li><a href="103063?version=1&table=Table 628">1/SIG*D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 628) <li><a href="103063?version=1&table=Table 629">1/SIG*D2SIG/DT1_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 629) <li><a href="103063?version=1&table=Table 630">1/SIG*D2SIG/DT1_PT/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 630) <li><a href="103063?version=1&table=Table 637">D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 637) <li><a href="103063?version=1&table=Table 638">D2SIG/DT1_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 638) <li><a href="103063?version=1&table=Table 639">D2SIG/DT1_PT/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 639) <li><a href="103063?version=1&table=Table 646">1/SIG*D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 170.0 GeV)</a> (Table 646) <li><a href="103063?version=1&table=Table 647">1/SIG*D2SIG/DT1_PT/DT2_PT ( 170.0 GeV < T2_PT < 290.0 GeV)</a> (Table 647) <li><a href="103063?version=1&table=Table 648">1/SIG*D2SIG/DT1_PT/DT2_PT ( 290.0 GeV < T2_PT < 450.0 GeV)</a> (Table 648) <li><a href="103063?version=1&table=Table 649">1/SIG*D2SIG/DT1_PT/DT2_PT ( 450.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 649) <li><a href="103063?version=1&table=Table 660">D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 170.0 GeV)</a> (Table 660) <li><a href="103063?version=1&table=Table 661">D2SIG/DT1_PT/DT2_PT ( 170.0 GeV < T2_PT < 290.0 GeV)</a> (Table 661) <li><a href="103063?version=1&table=Table 662">D2SIG/DT1_PT/DT2_PT ( 290.0 GeV < T2_PT < 450.0 GeV)</a> (Table 662) <li><a href="103063?version=1&table=Table 663">D2SIG/DT1_PT/DT2_PT ( 450.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 663) </ul><br/> Covariances:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 493">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 493) <li><a href="103063?version=1&table=Table 494">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 494) <li><a href="103063?version=1&table=Table 495">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 495) <li><a href="103063?version=1&table=Table 496">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 496) <li><a href="103063?version=1&table=Table 497">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 497) <li><a href="103063?version=1&table=Table 498">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 498) <li><a href="103063?version=1&table=Table 502">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 502) <li><a href="103063?version=1&table=Table 503">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 503) <li><a href="103063?version=1&table=Table 504">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 504) <li><a href="103063?version=1&table=Table 505">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 505) <li><a href="103063?version=1&table=Table 506">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 506) <li><a href="103063?version=1&table=Table 507">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 507) <li><a href="103063?version=1&table=Table 512">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 1th and 1th bins of ABS_T1_Y</a> (Table 512) <li><a href="103063?version=1&table=Table 513">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 1th bins of ABS_T1_Y</a> (Table 513) <li><a href="103063?version=1&table=Table 514">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 2th bins of ABS_T1_Y</a> (Table 514) <li><a href="103063?version=1&table=Table 515">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 1th bins of ABS_T1_Y</a> (Table 515) <li><a href="103063?version=1&table=Table 516">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 2th bins of ABS_T1_Y</a> (Table 516) <li><a href="103063?version=1&table=Table 517">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 3th bins of ABS_T1_Y</a> (Table 517) <li><a href="103063?version=1&table=Table 518">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 1th bins of ABS_T1_Y</a> (Table 518) <li><a href="103063?version=1&table=Table 519">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 2th bins of ABS_T1_Y</a> (Table 519) <li><a href="103063?version=1&table=Table 520">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 3th bins of ABS_T1_Y</a> (Table 520) <li><a href="103063?version=1&table=Table 521">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 4th bins of ABS_T1_Y</a> (Table 521) <li><a href="103063?version=1&table=Table 526">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 1th and 1th bins of ABS_T1_Y</a> (Table 526) <li><a href="103063?version=1&table=Table 527">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 1th bins of ABS_T1_Y</a> (Table 527) <li><a href="103063?version=1&table=Table 528">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 2th bins of ABS_T1_Y</a> (Table 528) <li><a href="103063?version=1&table=Table 529">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 1th bins of ABS_T1_Y</a> (Table 529) <li><a href="103063?version=1&table=Table 530">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 2th bins of ABS_T1_Y</a> (Table 530) <li><a href="103063?version=1&table=Table 531">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 3th bins of ABS_T1_Y</a> (Table 531) <li><a href="103063?version=1&table=Table 532">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 1th bins of ABS_T1_Y</a> (Table 532) <li><a href="103063?version=1&table=Table 533">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 2th bins of ABS_T1_Y</a> (Table 533) <li><a href="103063?version=1&table=Table 534">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 3th bins of ABS_T1_Y</a> (Table 534) <li><a href="103063?version=1&table=Table 535">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 4th bins of ABS_T1_Y</a> (Table 535) <li><a href="103063?version=1&table=Table 540">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 1th and 1th bins of M</a> (Table 540) <li><a href="103063?version=1&table=Table 541">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 2th and 1th bins of M</a> (Table 541) <li><a href="103063?version=1&table=Table 542">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 2th and 2th bins of M</a> (Table 542) <li><a href="103063?version=1&table=Table 543">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 1th bins of M</a> (Table 543) <li><a href="103063?version=1&table=Table 544">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 2th bins of M</a> (Table 544) <li><a href="103063?version=1&table=Table 545">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 3th bins of M</a> (Table 545) <li><a href="103063?version=1&table=Table 546">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 1th bins of M</a> (Table 546) <li><a href="103063?version=1&table=Table 547">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 2th bins of M</a> (Table 547) <li><a href="103063?version=1&table=Table 548">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 3th bins of M</a> (Table 548) <li><a href="103063?version=1&table=Table 549">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 4th bins of M</a> (Table 549) <li><a href="103063?version=1&table=Table 554">Matrix for D2SIG/DT2_PT/DM between the 1th and 1th bins of M</a> (Table 554) <li><a href="103063?version=1&table=Table 555">Matrix for D2SIG/DT2_PT/DM between the 2th and 1th bins of M</a> (Table 555) <li><a href="103063?version=1&table=Table 556">Matrix for D2SIG/DT2_PT/DM between the 2th and 2th bins of M</a> (Table 556) <li><a href="103063?version=1&table=Table 557">Matrix for D2SIG/DT2_PT/DM between the 3th and 1th bins of M</a> (Table 557) <li><a href="103063?version=1&table=Table 558">Matrix for D2SIG/DT2_PT/DM between the 3th and 2th bins of M</a> (Table 558) <li><a href="103063?version=1&table=Table 559">Matrix for D2SIG/DT2_PT/DM between the 3th and 3th bins of M</a> (Table 559) <li><a href="103063?version=1&table=Table 560">Matrix for D2SIG/DT2_PT/DM between the 4th and 1th bins of M</a> (Table 560) <li><a href="103063?version=1&table=Table 561">Matrix for D2SIG/DT2_PT/DM between the 4th and 2th bins of M</a> (Table 561) <li><a href="103063?version=1&table=Table 562">Matrix for D2SIG/DT2_PT/DM between the 4th and 3th bins of M</a> (Table 562) <li><a href="103063?version=1&table=Table 563">Matrix for D2SIG/DT2_PT/DM between the 4th and 4th bins of M</a> (Table 563) <li><a href="103063?version=1&table=Table 567">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 567) <li><a href="103063?version=1&table=Table 568">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 568) <li><a href="103063?version=1&table=Table 569">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 569) <li><a href="103063?version=1&table=Table 570">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 570) <li><a href="103063?version=1&table=Table 571">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 571) <li><a href="103063?version=1&table=Table 572">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 572) <li><a href="103063?version=1&table=Table 576">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 576) <li><a href="103063?version=1&table=Table 577">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 577) <li><a href="103063?version=1&table=Table 578">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 578) <li><a href="103063?version=1&table=Table 579">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 579) <li><a href="103063?version=1&table=Table 580">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 580) <li><a href="103063?version=1&table=Table 581">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 581) <li><a href="103063?version=1&table=Table 585">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 585) <li><a href="103063?version=1&table=Table 586">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 586) <li><a href="103063?version=1&table=Table 587">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 587) <li><a href="103063?version=1&table=Table 588">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 588) <li><a href="103063?version=1&table=Table 589">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 589) <li><a href="103063?version=1&table=Table 590">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 590) <li><a href="103063?version=1&table=Table 594">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 594) <li><a href="103063?version=1&table=Table 595">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 595) <li><a href="103063?version=1&table=Table 596">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 596) <li><a href="103063?version=1&table=Table 597">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 597) <li><a href="103063?version=1&table=Table 598">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 598) <li><a href="103063?version=1&table=Table 599">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 599) <li><a href="103063?version=1&table=Table 604">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 604) <li><a href="103063?version=1&table=Table 605">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 605) <li><a href="103063?version=1&table=Table 606">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 606) <li><a href="103063?version=1&table=Table 607">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 607) <li><a href="103063?version=1&table=Table 608">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 608) <li><a href="103063?version=1&table=Table 609">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 609) <li><a href="103063?version=1&table=Table 610">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 610) <li><a href="103063?version=1&table=Table 611">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 611) <li><a href="103063?version=1&table=Table 612">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 612) <li><a href="103063?version=1&table=Table 613">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 613) <li><a href="103063?version=1&table=Table 618">Matrix for D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 618) <li><a href="103063?version=1&table=Table 619">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 619) <li><a href="103063?version=1&table=Table 620">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 620) <li><a href="103063?version=1&table=Table 621">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 621) <li><a href="103063?version=1&table=Table 622">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 622) <li><a href="103063?version=1&table=Table 623">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 623) <li><a href="103063?version=1&table=Table 624">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 624) <li><a href="103063?version=1&table=Table 625">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 625) <li><a href="103063?version=1&table=Table 626">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 626) <li><a href="103063?version=1&table=Table 627">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 627) <li><a href="103063?version=1&table=Table 631">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 631) <li><a href="103063?version=1&table=Table 632">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 632) <li><a href="103063?version=1&table=Table 633">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 633) <li><a href="103063?version=1&table=Table 634">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 634) <li><a href="103063?version=1&table=Table 635">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 635) <li><a href="103063?version=1&table=Table 636">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 636) <li><a href="103063?version=1&table=Table 640">Matrix for D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 640) <li><a href="103063?version=1&table=Table 641">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 641) <li><a href="103063?version=1&table=Table 642">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 642) <li><a href="103063?version=1&table=Table 643">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 643) <li><a href="103063?version=1&table=Table 644">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 644) <li><a href="103063?version=1&table=Table 645">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 645) <li><a href="103063?version=1&table=Table 650">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 650) <li><a href="103063?version=1&table=Table 651">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 651) <li><a href="103063?version=1&table=Table 652">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 652) <li><a href="103063?version=1&table=Table 653">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 653) <li><a href="103063?version=1&table=Table 654">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 654) <li><a href="103063?version=1&table=Table 655">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 655) <li><a href="103063?version=1&table=Table 656">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 656) <li><a href="103063?version=1&table=Table 657">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 657) <li><a href="103063?version=1&table=Table 658">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 658) <li><a href="103063?version=1&table=Table 659">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 659) <li><a href="103063?version=1&table=Table 664">Matrix for D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 664) <li><a href="103063?version=1&table=Table 665">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 665) <li><a href="103063?version=1&table=Table 666">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 666) <li><a href="103063?version=1&table=Table 667">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 667) <li><a href="103063?version=1&table=Table 668">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 668) <li><a href="103063?version=1&table=Table 669">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 669) <li><a href="103063?version=1&table=Table 670">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 670) <li><a href="103063?version=1&table=Table 671">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 671) <li><a href="103063?version=1&table=Table 672">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 672) <li><a href="103063?version=1&table=Table 673">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 673) </ul><br/>

Relative differential cross-section as a function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.

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Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in pp collisions at $\sqrt{s} =$ 13 TeV

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
JHEP 06 (2020) 146, 2020.
Inspire Record 1772050 DOI 10.17182/hepdata.95469

The parton-level top quark (t) forward-backward asymmetry and the anomalous chromoelectric ($\hat{d}_\mathrm{t}$) and chromomagnetic ($\hat{\mu}_\mathrm{t}$) moments have been measured using LHC pp collisions at a center-of-mass energy of 13 TeV, collected in the CMS detector in a data sample corresponding to an integrated luminosity of 35.9 fb$^{-1}$. The linearized variable $A_\mathrm{FB}^{(1)}$ is used to approximate the asymmetry. Candidate $\mathrm{t\bar{t}}$ events decaying to a muon or electron and jets in final states with low and high Lorentz boosts are selected and reconstructed using a fit of the kinematic distributions of the decay products to those expected for $\mathrm{t\bar{t}}$ final states. The values found for the parameters are $A_\mathrm{FB}^{(1)} =$ 0.048 $^{+0.095}_{-0.087}$ (stat) $^{+0.020}_{-0.029}$ (syst), $\hat{\mu}_\mathrm{t} =-$ 0.024 $^{+0.013}_{-0.009}$ (stat) $^{+0.016}_{-0.011}$ (syst), and a limit is placed on the magnitude of $|\hat{d}_\mathrm{t}|$ $<$ 0.03 at 95% confidence level.

3 data tables

Linearized top quark forward-backward production asymmetry $A_{FB}^{(1)}$

Top quark anomalous chromomagnetic dipole moment $\hat{\mu}_{t}$

Top quark anomalous chromoelectric dipole moment $\hat{d}_{t}$


Measurement of the top quark pair production cross section in dilepton final states containing one $\tau$ lepton in pp collisions at $\sqrt{s}=$ 13 TeV

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
JHEP 02 (2020) 191, 2020.
Inspire Record 1767671 DOI 10.17182/hepdata.93743

The cross section of top quark pair production is measured in the $\mathrm{t\bar{t}}\to (\ell\nu_{\ell})(\tau_\mathrm{h}\nu_{\tau})\mathrm{b\bar{b}}$ final state, where $\tau_\mathrm{h}$ refers to the hadronic decays of the $\tau$ lepton, and $\ell$ is either an electron or a muon. The data sample corresponds to an integrated luminosity of 35.9 fb$^{-1}$ collected in proton-proton collisions at $\sqrt{s}=$ 13 TeV with the CMS detector. The measured cross section is $\sigma_{\mathrm{t\bar{t}}} =$ 781 $\pm$ 7 (stat) $\pm$ 62 (syst) $\pm$ 20 (lum) pb, and the ratio of the partial width $\Gamma($t$\to\tau\nu_{\tau}$b) to the total decay width of the top quark is measured to be 0.1050 $\pm$ 0.0009 (stat) $\pm$ 0.0071 (syst). This is the first measurement of the $\mathrm{t\bar{t}}$ production cross section in proton-proton collisions at $\sqrt{s}=$ 13 TeV that explicitly includes $\tau$ leptons. The ratio of the cross sections in the $\ell\tau_\mathrm{h}$ and $\ell\ell$ final states yields a value $R_{\ell\tau_\mathrm{h}/\ell\ell}=$ 0.973 $\pm$ 0.009 (stat) $\pm$ 0.066 (syst), consistent with lepton universality.

3 data tables

The measured inclusive top quark pair production cross section in the dilepton final state with one tau lepton.

The ratio between top quark production cross sections measured in lepton-tau and light dilepton final states.

The ratio of the partial width to the total decay width of the top quark.


Measurements of top-quark pair differential and double-differential cross-sections in the $\ell$+jets channel with $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
Eur.Phys.J.C 79 (2019) 1028, 2019.
Inspire Record 1750330 DOI 10.17182/hepdata.95758

Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\mathrm{fb}^{-1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.

1129 data tables

- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definitions:</b><br/> <i>Resolved:</i> <ul> <li> NLEP = 1, either E or MU, PT &gt; 27 GeV, ABS ETA &lt; 2.5 <li> NJETS &gt;= 4, PT &gt; 25 GeV, ABS ETA &lt; 2.5 <li> NBJETS &gt;= 2 </ul><br/> <i>Boosted:</i> <ul> <li> NLEP = 1, either E or MU, PT &gt; 27 GeV, ABS ETA &lt; 2.5 <li> NJETS &gt;= 1, R = 0.4, PT &gt; 25 GeV, ABS ETA &lt; 2.5 <li> NBJETS &gt;= 1 <li> NJETS &gt;= 1, R=1, PT &gt; 350 GeV, ABS ETA &lt; 2.0, top-tagged </ul><br/> <b>Particle level:</b><br/> <i>Resolved:</i><br/> <u>1D:</u><br/> Spectra: <ul> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1">Table 1</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 3">Table 3</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 5">Table 5</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 7">Table 7</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 9">Table 9</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 11">Table 11</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 13">Table 13</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 15">Table 15</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 17">Table 17</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 19">Table 19</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 21">Table 21</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 23">Table 23</a> ) <li>1/SIG*DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 25">Table 25</a> ) <li>DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 27">Table 27</a> ) <li>1/SIG*DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 29">Table 29</a> ) <li>DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 31">Table 31</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 33">Table 33</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 35">Table 35</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 37">Table 37</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 39">Table 39</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 41">Table 41</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 43">Table 43</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 45">Table 45</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 47">Table 47</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 49">Table 49</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 51">Table 51</a> ) <li>SIG (<a href="95758?version=1&table=Table 53">Table 53</a> ) </ul><br/> Covariances: <ul> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 2">Table 2</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 4">Table 4</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 6">Table 6</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 8">Table 8</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 10">Table 10</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 12">Table 12</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 14">Table 14</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 16">Table 16</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 18">Table 18</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 20">Table 20</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 22">Table 22</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 24">Table 24</a> ) <li>1/SIG*DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 26">Table 26</a> ) <li>DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 28">Table 28</a> ) <li>1/SIG*DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 30">Table 30</a> ) <li>DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 32">Table 32</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 34">Table 34</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 36">Table 36</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 38">Table 38</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 40">Table 40</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 42">Table 42</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 44">Table 44</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 46">Table 46</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 48">Table 48</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 50">Table 50</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 52">Table 52</a> ) </ul><br/> Inter-spectra correlations: <ul> <li>Statistical correlation between DSIG/DPT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 518">Table 518</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 519">Table 519</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 520">Table 520</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 521">Table 521</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 522">Table 522</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 523">Table 523</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 524">Table 524</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 525">Table 525</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 526">Table 526</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 527">Table 527</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 528">Table 528</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 529">Table 529</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 530">Table 530</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 531">Table 531</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 532">Table 532</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 533">Table 533</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 534">Table 534</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 535">Table 535</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 536">Table 536</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 537">Table 537</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 538">Table 538</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 539">Table 539</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 540">Table 540</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 541">Table 541</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 542">Table 542</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 543">Table 543</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 544">Table 544</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 545">Table 545</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 546">Table 546</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 547">Table 547</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 548">Table 548</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 549">Table 549</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 550">Table 550</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 551">Table 551</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 552">Table 552</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 553">Table 553</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 554">Table 554</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 555">Table 555</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 556">Table 556</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 557">Table 557</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 558">Table 558</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 559">Table 559</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 560">Table 560</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 561">Table 561</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 562">Table 562</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 563">Table 563</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 564">Table 564</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 565">Table 565</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 566">Table 566</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 567">Table 567</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 568">Table 568</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 569">Table 569</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 570">Table 570</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 571">Table 571</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 572">Table 572</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 573">Table 573</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 574">Table 574</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 575">Table 575</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 576">Table 576</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 577">Table 577</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 578">Table 578</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 579">Table 579</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 580">Table 580</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 581">Table 581</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 582">Table 582</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 583">Table 583</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 584">Table 584</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 585">Table 585</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 586">Table 586</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 587">Table 587</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 588">Table 588</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 589">Table 589</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 590">Table 590</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 591">Table 591</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 592">Table 592</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 593">Table 593</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 594">Table 594</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 595">Table 595</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 596">Table 596</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 597">Table 597</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 598">Table 598</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 599">Table 599</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 600">Table 600</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 601">Table 601</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 602">Table 602</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 603">Table 603</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 604">Table 604</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 605">Table 605</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 606">Table 606</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 607">Table 607</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 608">Table 608</a> ) </ul><br/> <u>2D:</u><br/> Spectra: <ul> <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 54">Table 54</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 55">Table 55</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 56">Table 56</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 57">Table 57</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 58">Table 58</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 74">Table 74</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 75">Table 75</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 76">Table 76</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 77">Table 77</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 78">Table 78</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 94">Table 94</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 95">Table 95</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 96">Table 96</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 97">Table 97</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 98">Table 98</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 114">Table 114</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 115">Table 115</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 116">Table 116</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 117">Table 117</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 118">Table 118</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 0.0 GeV < PT_THAD < 60.0 GeV) (<a href="95758?version=1&table=Table 134">Table 134</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 60.0 GeV < PT_THAD < 120.0 GeV) (<a href="95758?version=1&table=Table 135">Table 135</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 120.0 GeV < PT_THAD < 200.0 GeV) (<a href="95758?version=1&table=Table 136">Table 136</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 200.0 GeV < PT_THAD < 300.0 GeV) (<a href="95758?version=1&table=Table 137">Table 137</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 300.0 GeV < PT_THAD < 1000.0 GeV) (<a href="95758?version=1&table=Table 138">Table 138</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 0.0 GeV < PT_THAD < 60.0 GeV) (<a href="95758?version=1&table=Table 154">Table 154</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 60.0 GeV < PT_THAD < 120.0 GeV) (<a href="95758?version=1&table=Table 155">Table 155</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 120.0 GeV < PT_THAD < 200.0 GeV) (<a href="95758?version=1&table=Table 156">Table 156</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 200.0 GeV < PT_THAD < 300.0 GeV) (<a href="95758?version=1&table=Table 157">Table 157</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 300.0 GeV < PT_THAD < 1000.0 GeV) (<a href="95758?version=1&table=Table 158">Table 158</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 174">Table 174</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 175">Table 175</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 176">Table 176</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 177">Table 177</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 188">Table 188</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 189">Table 189</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 190">Table 190</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 191">Table 191</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 202">Table 202</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 203">Table 203</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS $\geq$ 6.0) (<a href="95758?version=1&table=Table 204">Table 204</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 211">Table 211</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 212">Table 212</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS $\geq$ 6.0) (<a href="95758?version=1&table=Table 213">Table 213</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 220">Table 220</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 221">Table 221</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 222">Table 222</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 223">Table 223</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 234">Table 234</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 235">Table 235</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 236">Table 236</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 237">Table 237</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 248">Table 248</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 249">Table 249</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 250">Table 250</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 251">Table 251</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 262">Table 262</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 263">Table 263</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 264">Table 264</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 265">Table 265</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 3.5 < N_JETS < 4.5 ) (<a href="95758?version=1&table=Table 276">Table 276</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 4.5 < N_JETS < 5.5 ) (<a href="95758?version=1&table=Table 277">Table 277</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 5.5 < N_JETS < 6.5 ) (<a href="95758?version=1&table=Table 278">Table 278</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 6.5 < N_JETS < 7.5 ) (<a href="95758?version=1&table=Table 279">Table 279</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 3.5 < N_JETS < 4.5 ) (<a href="95758?version=1&table=Table 290">Table 290</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 4.5 < N_JETS < 5.5 ) (<a href="95758?version=1&table=Table 291">Table 291</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 5.5 < N_JETS < 6.5 ) (<a href="95758?version=1&table=Table 292">Table 292</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 6.5 < N_JETS < 7.5 ) (<a href="95758?version=1&table=Table 293">Table 293</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 304">Table 304</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 305">Table 305</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 306">Table 306</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 307">Table 307</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 318">Table 318</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 319">Table 319</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 320">Table 320</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 321">Table 321</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 332">Table 332</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 333">Table 333</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 334">Table 334</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 335">Table 335</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 346">Table 346</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 347">Table 347</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 348">Table 348</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 349">Table 349</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 360">Table 360</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 361">Table 361</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 362">Table 362</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 363">Table 363</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 374">Table 374</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 375">Table 375</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 376">Table 376</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 377">Table 377</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 388">Table 388</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 389">Table 389</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 390">Table 390</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 391">Table 391</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 402">Table 402</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 403">Table 403</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 404">Table 404</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 405">Table 405</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 0.7 ) (<a href="95758?version=1&table=Table 416">Table 416</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.7 < ABS_Y_THAD < 1.4 ) (<a href="95758?version=1&table=Table 417">Table 417</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 1.4 < ABS_Y_THAD < 2.5 ) (<a href="95758?version=1&table=Table 418">Table 418</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 0.7 ) (<a href="95758?version=1&table=Table 425">Table 425</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.7 < ABS_Y_THAD < 1.4 ) (<a href="95758?version=1&table=Table 426">Table 426</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 1.4 < ABS_Y_THAD < 2.5 ) (<a href="95758?version=1&table=Table 427">Table 427</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 434">Table 434</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 435">Table 435</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 436">Table 436</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 437">Table 437</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 448">Table 448</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 449">Table 449</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 450">Table 450</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 451">Table 451</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 462">Table 462</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 463">Table 463</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 464">Table 464</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 465">Table 465</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 476">Table 476</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 477">Table 477</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 478">Table 478</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 479">Table 479</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 30.0 GeV) (<a href="95758?version=1&table=Table 490">Table 490</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 30.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 491">Table 491</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 190.0 GeV) (<a href="95758?version=1&table=Table 492">Table 492</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 190.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 493">Table 493</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 30.0 GeV) (<a href="95758?version=1&table=Table 504">Table 504</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 30.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 505">Table 505</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 190.0 GeV) (<a href="95758?version=1&table=Table 506">Table 506</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 190.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 507">Table 507</a> ) </ul><br/> Covariances:<br/><ul> <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 59">Table 59</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 60">Table 60</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 61">Table 61</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 62">Table 62</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 63">Table 63</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 64">Table 64</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 65">Table 65</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 66">Table 66</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 67">Table 67</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 68">Table 68</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 69">Table 69</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 70">Table 70</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 71">Table 71</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 72">Table 72</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 73">Table 73</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 79">Table 79</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 80">Table 80</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 81">Table 81</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 82">Table 82</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 83">Table 83</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 84">Table 84</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 85">Table 85</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 86">Table 86</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 87">Table 87</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 88">Table 88</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 89">Table 89</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 90">Table 90</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 91">Table 91</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 92">Table 92</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 93">Table 93</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 99">Table 99</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 100">Table 100</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 101">Table 101</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 102">Table 102</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 103">Table 103</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 104">Table 104</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 105">Table 105</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 106">Table 106</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 107">Table 107</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 108">Table 108</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 109">Table 109</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 110">Table 110</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 111">Table 111</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 112">Table 112</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 113">Table 113</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 119">Table 119</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 120">Table 120</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 121">Table 121</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 122">Table 122</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 123">Table 123</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 124">Table 124</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 125">Table 125</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 126">Table 126</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 127">Table 127</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 128">Table 128</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 129">Table 129</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 130">Table 130</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 131">Table 131</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 132">Table 132</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 133">Table 133</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 1th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 139">Table 139</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 140">Table 140</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 141">Table 141</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 142">Table 142</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 143">Table 143</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 144">Table 144</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 145">Table 145</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 146">Table 146</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 147">Table 147</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 148">Table 148</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 149">Table 149</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 150">Table 150</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 151">Table 151</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 152">Table 152</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 5th bins of PT_THAD (<a href="95758?version=1&table=Table 153">Table 153</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 1th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 159">Table 159</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 160">Table 160</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 161">Table 161</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 162">Table 162</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 163">Table 163</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 164">Table 164</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 165">Table 165</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 166">Table 166</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 167">Table 167</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 168">Table 168</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 169">Table 169</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 170">Table 170</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 171">Table 171</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 172">Table 172</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 5th bins of PT_THAD (<a href="95758?version=1&table=Table 173">Table 173</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 178">Table 178</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 179">Table 179</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 180">Table 180</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 181">Table 181</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 182">Table 182</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 183">Table 183</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 184">Table 184</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 185">Table 185</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 186">Table 186</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 187">Table 187</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 192">Table 192</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 193">Table 193</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 194">Table 194</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 195">Table 195</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 196">Table 196</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 197">Table 197</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 198">Table 198</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 199">Table 199</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 200">Table 200</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 201">Table 201</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 205">Table 205</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 206">Table 206</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 207">Table 207</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 208">Table 208</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 209">Table 209</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 210">Table 210</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 214">Table 214</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 215">Table 215</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 216">Table 216</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 217">Table 217</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 218">Table 218</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 219">Table 219</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 224">Table 224</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 225">Table 225</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 226">Table 226</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 227">Table 227</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 228">Table 228</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 229">Table 229</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 230">Table 230</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 231">Table 231</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 232">Table 232</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 233">Table 233</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 238">Table 238</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 239">Table 239</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 240">Table 240</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 241">Table 241</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 242">Table 242</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 243">Table 243</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 244">Table 244</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 245">Table 245</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 246">Table 246</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 247">Table 247</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 252">Table 252</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 253">Table 253</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 254">Table 254</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 255">Table 255</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 256">Table 256</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 257">Table 257</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 258">Table 258</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 259">Table 259</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 260">Table 260</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 261">Table 261</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 266">Table 266</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 267">Table 267</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 268">Table 268</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 269">Table 269</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 270">Table 270</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 271">Table 271</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 272">Table 272</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 273">Table 273</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 274">Table 274</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 275">Table 275</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 280">Table 280</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 281">Table 281</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 282">Table 282</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 283">Table 283</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 284">Table 284</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 285">Table 285</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 286">Table 286</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 287">Table 287</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 288">Table 288</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 289">Table 289</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 294">Table 294</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 295">Table 295</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 296">Table 296</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 297">Table 297</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 298">Table 298</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 299">Table 299</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 300">Table 300</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 301">Table 301</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 302">Table 302</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 303">Table 303</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 308">Table 308</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 309">Table 309</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 310">Table 310</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 311">Table 311</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 312">Table 312</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 313">Table 313</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 314">Table 314</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 315">Table 315</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 316">Table 316</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 317">Table 317</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 322">Table 322</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 323">Table 323</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 324">Table 324</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 325">Table 325</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 326">Table 326</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 327">Table 327</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 328">Table 328</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 329">Table 329</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 330">Table 330</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 331">Table 331</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 336">Table 336</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 337">Table 337</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 338">Table 338</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 339">Table 339</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 340">Table 340</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 341">Table 341</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 342">Table 342</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 343">Table 343</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 344">Table 344</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 345">Table 345</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 350">Table 350</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 351">Table 351</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 352">Table 352</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 353">Table 353</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 354">Table 354</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 355">Table 355</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 356">Table 356</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 357">Table 357</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 358">Table 358</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 359">Table 359</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 364">Table 364</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 365">Table 365</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 366">Table 366</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 367">Table 367</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 368">Table 368</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 369">Table 369</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 370">Table 370</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 371">Table 371</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 372">Table 372</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 373">Table 373</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 378">Table 378</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 379">Table 379</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 380">Table 380</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 381">Table 381</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 382">Table 382</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 383">Table 383</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 384">Table 384</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 385">Table 385</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 386">Table 386</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 387">Table 387</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 392">Table 392</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 393">Table 393</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 394">Table 394</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 395">Table 395</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 396">Table 396</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 397">Table 397</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 398">Table 398</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 399">Table 399</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 400">Table 400</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 401">Table 401</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 406">Table 406</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 407">Table 407</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 408">Table 408</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 409">Table 409</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 410">Table 410</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 411">Table 411</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 412">Table 412</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 413">Table 413</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 414">Table 414</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 415">Table 415</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 419">Table 419</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 420">Table 420</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 421">Table 421</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 422">Table 422</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 423">Table 423</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 3th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 424">Table 424</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 428">Table 428</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 429">Table 429</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 430">Table 430</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 431">Table 431</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 432">Table 432</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 3th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 433">Table 433</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 438">Table 438</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 439">Table 439</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 440">Table 440</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 441">Table 441</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 442">Table 442</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 443">Table 443</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 444">Table 444</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 445">Table 445</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 446">Table 446</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 447">Table 447</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 452">Table 452</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 453">Table 453</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 454">Table 454</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 455">Table 455</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 456">Table 456</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 457">Table 457</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 458">Table 458</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 459">Table 459</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 460">Table 460</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 461">Table 461</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 466">Table 466</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 467">Table 467</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 468">Table 468</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 469">Table 469</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 470">Table 470</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 471">Table 471</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 472">Table 472</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 473">Table 473</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 474">Table 474</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 475">Table 475</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 480">Table 480</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 481">Table 481</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 482">Table 482</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 483">Table 483</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 484">Table 484</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 485">Table 485</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 486">Table 486</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 487">Table 487</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 488">Table 488</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 489">Table 489</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 494">Table 494</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 495">Table 495</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 496">Table 496</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 497">Table 497</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 498">Table 498</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 499">Table 499</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 500">Table 500</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 501">Table 501</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 502">Table 502</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 503">Table 503</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 508">Table 508</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 509">Table 509</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 510">Table 510</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 511">Table 511</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 512">Table 512</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 513">Table 513</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 514">Table 514</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 515">Table 515</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 516">Table 516</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 517">Table 517</a> ) </ul><br/> <i>Boosted:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 840">Table 840</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 842">Table 842</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 844">Table 844</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 846">Table 846</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 848">Table 848</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 850">Table 850</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 852">Table 852</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 854">Table 854</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 856">Table 856</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 858">Table 858</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 860">Table 860</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 862">Table 862</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 864">Table 864</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 866">Table 866</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 868">Table 868</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 870">Table 870</a> ) <li>1/SIG*DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 872">Table 872</a> ) <li>DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 874">Table 874</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 876">Table 876</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 878">Table 878</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 880">Table 880</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 882">Table 882</a> ) <li>1/SIG*DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 884">Table 884</a> ) <li>DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 886">Table 886</a> ) <li>SIG (<a href="95758?version=1&table=Table 888">Table 888</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 841">Table 841</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 843">Table 843</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 845">Table 845</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 847">Table 847</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 849">Table 849</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 851">Table 851</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 853">Table 853</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 855">Table 855</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 857">Table 857</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 859">Table 859</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 861">Table 861</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 863">Table 863</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 865">Table 865</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 867">Table 867</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 869">Table 869</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 871">Table 871</a> ) <li>1/SIG*DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 873">Table 873</a> ) <li>DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 875">Table 875</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 877">Table 877</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 879">Table 879</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 881">Table 881</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 883">Table 883</a> ) <li>1/SIG*DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 885">Table 885</a> ) <li>DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 887">Table 887</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DPT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1029">Table 1029</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1030">Table 1030</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1031">Table 1031</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1032">Table 1032</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1033">Table 1033</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1034">Table 1034</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1035">Table 1035</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1036">Table 1036</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1037">Table 1037</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1038">Table 1038</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1039">Table 1039</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1040">Table 1040</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1041">Table 1041</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1042">Table 1042</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1043">Table 1043</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1044">Table 1044</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1045">Table 1045</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1046">Table 1046</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1047">Table 1047</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1048">Table 1048</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1049">Table 1049</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1050">Table 1050</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1051">Table 1051</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1052">Table 1052</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1053">Table 1053</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1054">Table 1054</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1055">Table 1055</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1056">Table 1056</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1057">Table 1057</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1058">Table 1058</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1059">Table 1059</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1060">Table 1060</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1061">Table 1061</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1062">Table 1062</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1063">Table 1063</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1064">Table 1064</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1065">Table 1065</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1066">Table 1066</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1067">Table 1067</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1068">Table 1068</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1069">Table 1069</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1070">Table 1070</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1071">Table 1071</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1072">Table 1072</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1073">Table 1073</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1074">Table 1074</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1075">Table 1075</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1076">Table 1076</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1077">Table 1077</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1078">Table 1078</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1079">Table 1079</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1080">Table 1080</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1081">Table 1081</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1082">Table 1082</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1083">Table 1083</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1084">Table 1084</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1085">Table 1085</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1086">Table 1086</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1087">Table 1087</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1088">Table 1088</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1089">Table 1089</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1090">Table 1090</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1091">Table 1091</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1092">Table 1092</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1093">Table 1093</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 1094">Table 1094</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1095">Table 1095</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1096">Table 1096</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1097">Table 1097</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1098">Table 1098</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1099">Table 1099</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1100">Table 1100</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1101">Table 1101</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1102">Table 1102</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1103">Table 1103</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1104">Table 1104</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 1105">Table 1105</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 1106">Table 1106</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 889">Table 889</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 890">Table 890</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 891">Table 891</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 898">Table 898</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 899">Table 899</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 900">Table 900</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 1.0 ) (<a href="95758?version=1&table=Table 907">Table 907</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR ( 1.0 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 908">Table 908</a> ) <li>D2SIG/DPT_THAD/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 1.0 ) (<a href="95758?version=1&table=Table 912">Table 912</a> ) <li>D2SIG/DPT_THAD/DABS_Y_TTBAR ( 1.0 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 913">Table 913</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 1.0 ) (<a href="95758?version=1&table=Table 917">Table 917</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 1.0 < ABS_Y_THAD < 2.0 ) (<a href="95758?version=1&table=Table 918">Table 918</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 1.0 ) (<a href="95758?version=1&table=Table 922">Table 922</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 1.0 < ABS_Y_THAD < 2.0 ) (<a href="95758?version=1&table=Table 923">Table 923</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 490.0 GeV < M_TTBAR < 1160.0 GeV) (<a href="95758?version=1&table=Table 927">Table 927</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 1160.0 GeV < M_TTBAR < 3000.0 GeV) (<a href="95758?version=1&table=Table 928">Table 928</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 490.0 GeV < M_TTBAR < 1160.0 GeV) (<a href="95758?version=1&table=Table 932">Table 932</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 1160.0 GeV < M_TTBAR < 3000.0 GeV) (<a href="95758?version=1&table=Table 933">Table 933</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR ( 350.0 GeV < HT_TTBAR < 780.0 GeV) (<a href="95758?version=1&table=Table 937">Table 937</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR ( 780.0 GeV < HT_TTBAR < 2500.0 GeV) (<a href="95758?version=1&table=Table 938">Table 938</a> ) <li>D2SIG/DM_TTBAR/DHT_TTBAR ( 350.0 GeV < HT_TTBAR < 780.0 GeV) (<a href="95758?version=1&table=Table 942">Table 942</a> ) <li>D2SIG/DM_TTBAR/DHT_TTBAR ( 780.0 GeV < HT_TTBAR < 2500.0 GeV) (<a href="95758?version=1&table=Table 943">Table 943</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 947">Table 947</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 948">Table 948</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 949">Table 949</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 956">Table 956</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 957">Table 957</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 958">Table 958</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.65 ) (<a href="95758?version=1&table=Table 965">Table 965</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.65 < ABS_Y_TTBAR < 1.3 ) (<a href="95758?version=1&table=Table 966">Table 966</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.3 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 967">Table 967</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.65 ) (<a href="95758?version=1&table=Table 974">Table 974</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.65 < ABS_Y_TTBAR < 1.3 ) (<a href="95758?version=1&table=Table 975">Table 975</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.3 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 976">Table 976</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 983">Table 983</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 2.0) (<a href="95758?version=1&table=Table 984">Table 984</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 3.0) (<a href="95758?version=1&table=Table 985">Table 985</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 992">Table 992</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 2.0) (<a href="95758?version=1&table=Table 993">Table 993</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 3.0) (<a href="95758?version=1&table=Table 994">Table 994</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 1001">Table 1001</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.5) (<a href="95758?version=1&table=Table 1002">Table 1002</a> ) <li>D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 1006">Table 1006</a> ) <li>D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.5) (<a href="95758?version=1&table=Table 1007">Table 1007</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.0) (<a href="95758?version=1&table=Table 1011">Table 1011</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 1.0) (<a href="95758?version=1&table=Table 1012">Table 1012</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.0) (<a href="95758?version=1&table=Table 1013">Table 1013</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.0) (<a href="95758?version=1&table=Table 1020">Table 1020</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 1.0) (<a href="95758?version=1&table=Table 1021">Table 1021</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.0) (<a href="95758?version=1&table=Table 1022">Table 1022</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 892">Table 892</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 893">Table 893</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 894">Table 894</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 895">Table 895</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 896">Table 896</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 897">Table 897</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 901">Table 901</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 902">Table 902</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 903">Table 903</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 904">Table 904</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 905">Table 905</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 906">Table 906</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 909">Table 909</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 910">Table 910</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 911">Table 911</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 914">Table 914</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 915">Table 915</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 916">Table 916</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 919">Table 919</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 920">Table 920</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 921">Table 921</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 924">Table 924</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 925">Table 925</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 926">Table 926</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 929">Table 929</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 930">Table 930</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 931">Table 931</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 934">Table 934</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 935">Table 935</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 936">Table 936</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 1th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 939">Table 939</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 940">Table 940</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 2th bins of HT_TTBAR (<a href="95758?version=1&table=Table 941">Table 941</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 1th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 944">Table 944</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 945">Table 945</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 2th bins of HT_TTBAR (<a href="95758?version=1&table=Table 946">Table 946</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 950">Table 950</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 951">Table 951</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 952">Table 952</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 953">Table 953</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 954">Table 954</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 955">Table 955</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 959">Table 959</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 960">Table 960</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 961">Table 961</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 962">Table 962</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 963">Table 963</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 964">Table 964</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 968">Table 968</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 969">Table 969</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 970">Table 970</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 971">Table 971</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 972">Table 972</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 973">Table 973</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 977">Table 977</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 978">Table 978</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 979">Table 979</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 980">Table 980</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 981">Table 981</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 982">Table 982</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 986">Table 986</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 987">Table 987</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 988">Table 988</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 989">Table 989</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 990">Table 990</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 991">Table 991</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 995">Table 995</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 996">Table 996</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 997">Table 997</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 998">Table 998</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 999">Table 999</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1000">Table 1000</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1003">Table 1003</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1004">Table 1004</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1005">Table 1005</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1008">Table 1008</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1009">Table 1009</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1010">Table 1010</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1014">Table 1014</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1015">Table 1015</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1016">Table 1016</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1017">Table 1017</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1018">Table 1018</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1019">Table 1019</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1023">Table 1023</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1024">Table 1024</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1025">Table 1025</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1026">Table 1026</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1027">Table 1027</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1028">Table 1028</a> ) </ul><br/> <b>Parton level:</b><br/> <i>Resolved:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 609">Table 609</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 611">Table 611</a> ) <li>1/SIG*DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 613">Table 613</a> ) <li>DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 615">Table 615</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 617">Table 617</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 619">Table 619</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 621">Table 621</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 623">Table 623</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 625">Table 625</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 627">Table 627</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 629">Table 629</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 631">Table 631</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 633">Table 633</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 635">Table 635</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 637">Table 637</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 639">Table 639</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 610">Table 610</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 612">Table 612</a> ) <li>1/SIG*DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 614">Table 614</a> ) <li>DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 616">Table 616</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 618">Table 618</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 620">Table 620</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 622">Table 622</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 624">Table 624</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 626">Table 626</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 628">Table 628</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 630">Table 630</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 632">Table 632</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 634">Table 634</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 636">Table 636</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 638">Table 638</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 640">Table 640</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DPT_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 799">Table 799</a> ) <li>Statistical correlation between DSIG/DABS_Y_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 800">Table 800</a> ) <li>Statistical correlation between DSIG/DABS_Y_T and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 801">Table 801</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 802">Table 802</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 803">Table 803</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 804">Table 804</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 805">Table 805</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 806">Table 806</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 807">Table 807</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 808">Table 808</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 809">Table 809</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 810">Table 810</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 811">Table 811</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 812">Table 812</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 813">Table 813</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T (<a href="95758?version=1&table=Table 814">Table 814</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 815">Table 815</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 816">Table 816</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 817">Table 817</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 818">Table 818</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 819">Table 819</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 820">Table 820</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 821">Table 821</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 822">Table 822</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 823">Table 823</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 824">Table 824</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 825">Table 825</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 826">Table 826</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T (<a href="95758?version=1&table=Table 827">Table 827</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 828">Table 828</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 829">Table 829</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 830">Table 830</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 831">Table 831</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 832">Table 832</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 833">Table 833</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 834">Table 834</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 0.0 < ABS_Y_T < 0.75 ) (<a href="95758?version=1&table=Table 641">Table 641</a> ) <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 0.75 < ABS_Y_T < 1.5 ) (<a href="95758?version=1&table=Table 642">Table 642</a> ) <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 1.5 < ABS_Y_T < 2.5 ) (<a href="95758?version=1&table=Table 643">Table 643</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 0.0 < ABS_Y_T < 0.75 ) (<a href="95758?version=1&table=Table 650">Table 650</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 0.75 < ABS_Y_T < 1.5 ) (<a href="95758?version=1&table=Table 651">Table 651</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 1.5 < ABS_Y_T < 2.5 ) (<a href="95758?version=1&table=Table 652">Table 652</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 659">Table 659</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 180.0 GeV) (<a href="95758?version=1&table=Table 660">Table 660</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 180.0 GeV < PT_TTBAR < 330.0 GeV) (<a href="95758?version=1&table=Table 661">Table 661</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 330.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 662">Table 662</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 673">Table 673</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 180.0 GeV) (<a href="95758?version=1&table=Table 674">Table 674</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 180.0 GeV < PT_TTBAR < 330.0 GeV) (<a href="95758?version=1&table=Table 675">Table 675</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 330.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 676">Table 676</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 687">Table 687</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 688">Table 688</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 689">Table 689</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 690">Table 690</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 701">Table 701</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 702">Table 702</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 703">Table 703</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 704">Table 704</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 GeV < ABS_Y_TTBAR < 0.5 GeV) (<a href="95758?version=1&table=Table 715">Table 715</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 GeV < ABS_Y_TTBAR < 1.1 GeV) (<a href="95758?version=1&table=Table 716">Table 716</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 GeV < ABS_Y_TTBAR < 1.7 GeV) (<a href="95758?version=1&table=Table 717">Table 717</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 GeV < ABS_Y_TTBAR < 2.5 GeV) (<a href="95758?version=1&table=Table 718">Table 718</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 GeV < ABS_Y_TTBAR < 0.5 GeV) (<a href="95758?version=1&table=Table 729">Table 729</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 GeV < ABS_Y_TTBAR < 1.1 GeV) (<a href="95758?version=1&table=Table 730">Table 730</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 GeV < ABS_Y_TTBAR < 1.7 GeV) (<a href="95758?version=1&table=Table 731">Table 731</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 GeV < ABS_Y_TTBAR < 2.5 GeV) (<a href="95758?version=1&table=Table 732">Table 732</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 743">Table 743</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 744">Table 744</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 745">Table 745</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 746">Table 746</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 757">Table 757</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 758">Table 758</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 759">Table 759</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 760">Table 760</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.5 ) (<a href="95758?version=1&table=Table 771">Table 771</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 < ABS_Y_TTBAR < 1.1 ) (<a href="95758?version=1&table=Table 772">Table 772</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 < ABS_Y_TTBAR < 1.7 ) (<a href="95758?version=1&table=Table 773">Table 773</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 774">Table 774</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.5 ) (<a href="95758?version=1&table=Table 785">Table 785</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 < ABS_Y_TTBAR < 1.1 ) (<a href="95758?version=1&table=Table 786">Table 786</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 < ABS_Y_TTBAR < 1.7 ) (<a href="95758?version=1&table=Table 787">Table 787</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 788">Table 788</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 1th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 644">Table 644</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 2th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 645">Table 645</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 2th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 646">Table 646</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 647">Table 647</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 648">Table 648</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 3th bins of ABS_Y_T (<a href="95758?version=1&table=Table 649">Table 649</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 1th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 653">Table 653</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 2th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 654">Table 654</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 2th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 655">Table 655</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 656">Table 656</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 657">Table 657</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 3th bins of ABS_Y_T (<a href="95758?version=1&table=Table 658">Table 658</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 663">Table 663</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 664">Table 664</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 665">Table 665</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 666">Table 666</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 667">Table 667</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 668">Table 668</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 669">Table 669</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 670">Table 670</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 671">Table 671</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 672">Table 672</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 677">Table 677</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 678">Table 678</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 679">Table 679</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 680">Table 680</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 681">Table 681</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 682">Table 682</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 683">Table 683</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 684">Table 684</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 685">Table 685</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 686">Table 686</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 691">Table 691</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 692">Table 692</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 693">Table 693</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 694">Table 694</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 695">Table 695</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 696">Table 696</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 697">Table 697</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 698">Table 698</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 699">Table 699</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 700">Table 700</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 705">Table 705</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 706">Table 706</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 707">Table 707</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 708">Table 708</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 709">Table 709</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 710">Table 710</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 711">Table 711</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 712">Table 712</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 713">Table 713</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 714">Table 714</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 719">Table 719</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 720">Table 720</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 721">Table 721</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 722">Table 722</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 723">Table 723</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 724">Table 724</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 725">Table 725</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 726">Table 726</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 727">Table 727</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 728">Table 728</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 733">Table 733</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 734">Table 734</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 735">Table 735</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 736">Table 736</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 737">Table 737</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 738">Table 738</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 739">Table 739</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 740">Table 740</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 741">Table 741</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 742">Table 742</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 747">Table 747</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 748">Table 748</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 749">Table 749</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 750">Table 750</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 751">Table 751</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 752">Table 752</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 753">Table 753</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 754">Table 754</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 755">Table 755</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 756">Table 756</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 761">Table 761</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 762">Table 762</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 763">Table 763</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 764">Table 764</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 765">Table 765</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 766">Table 766</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 767">Table 767</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 768">Table 768</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 769">Table 769</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 770">Table 770</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 775">Table 775</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 776">Table 776</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 777">Table 777</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 778">Table 778</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 779">Table 779</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 780">Table 780</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 781">Table 781</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 782">Table 782</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 783">Table 783</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 784">Table 784</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 789">Table 789</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 790">Table 790</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 791">Table 791</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 792">Table 792</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 793">Table 793</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 794">Table 794</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 795">Table 795</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 796">Table 796</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 797">Table 797</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 798">Table 798</a> ) </ul><br/> <i>Resolved with CMS binning:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 835">Table 835</a> ) <li>DSIG/DY_T (<a href="95758?version=1&table=Table 836">Table 836</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 837">Table 837</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 838">Table 838</a> ) <li>DSIG/DY_TTBAR (<a href="95758?version=1&table=Table 839">Table 839</a> ) </ul><br/> <i>Boosted:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1107">Table 1107</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1109">Table 1109</a> ) <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 1111">Table 1111</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 1113">Table 1113</a> ) <li>SIG (<a href="95758?version=1&table=Table 1115">Table 1115</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1108">Table 1108</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1110">Table 1110</a> ) <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 1112">Table 1112</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 1114">Table 1114</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1126">Table 1126</a> ) <li>Statistical correlation between DSIG/DPT_T and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1127">Table 1127</a> ) <li>Statistical correlation between DSIG/DPT_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 1128">Table 1128</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DM_TTBAR/DPT_T ( 350.0 GeV < PT_T < 550.0 GeV) (<a href="95758?version=1&table=Table 1116">Table 1116</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T ( 550.0 GeV < PT_T < 2000.0 GeV) (<a href="95758?version=1&table=Table 1117">Table 1117</a> ) <li>D2SIG/DM_TTBAR/DPT_T ( 350.0 GeV < PT_T < 550.0 GeV) (<a href="95758?version=1&table=Table 1121">Table 1121</a> ) <li>D2SIG/DM_TTBAR/DPT_T ( 550.0 GeV < PT_T < 2000.0 GeV) (<a href="95758?version=1&table=Table 1122">Table 1122</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 1th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1118">Table 1118</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 2th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1119">Table 1119</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 2th and 2th bins of PT_T (<a href="95758?version=1&table=Table 1120">Table 1120</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 1th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1123">Table 1123</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 2th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1124">Table 1124</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 2th and 2th bins of PT_T (<a href="95758?version=1&table=Table 1125">Table 1125</a> ) </ul><br/>

Relative differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.

Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.

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Measurement of $K_S^0$ and $\Lambda^0$ production in $t \bar{t}$ dileptonic events in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
Eur.Phys.J.C 79 (2019) 1017, 2019.
Inspire Record 1746286 DOI 10.17182/hepdata.91243

Measurements of $K_S^0$ and $\Lambda^0$ production in $t\bar{t}$ final states have been performed. They are based on a data sample with integrated luminosity of 4.6 $\mathrm{fb}^{-1}$ from proton-proton collisions at a centre-of-mass energy of 7 TeV, collected in 2011 with the ATLAS detector at the Large Hadron Collider. Neutral strange particles are separated into three classes, depending on whether they are contained in a jet, with or without a $b$-tag, or not associated with a selected jet. The aim is to look for differences in their main kinematic distributions. A comparison of data with several Monte Carlo simulations using different hadronisation and fragmentation schemes, colour reconnection models and different tunes for the underlying event has been made. The production of neutral strange particles in $t\bar{t}$ dileptonic events is found to be well described by current Monte Carlo models for $K_S^0$ and $\Lambda^0$ production within jets, but not for those produced outside jets.

22 data tables

The transverse momentum ($p_{T}$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking inefficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The energy fraction ($x_{K}$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

The energy distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.

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Measurement of the top quark polarization and $\mathrm{t\bar{t}}$ spin correlations using dilepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
Phys.Rev.D 100 (2019) 072002, 2019.
Inspire Record 1742786 DOI 10.17182/hepdata.90640

Measurements of the top quark polarization and top quark pair ($\mathrm{t\bar{t}}$) spin correlations are presented using events containing two oppositely charged leptons (e$^+$e$^-$, e$^\pm\mu^\mp$, or $\mu^+\mu^-$) produced in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were recorded by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb$^{-1}$. A set of parton-level normalized differential cross sections, sensitive to each of the independent coefficients of the spin-dependent parts of the $\mathrm{t\bar{t}}$ production density matrix, is measured for the first time at 13 TeV. The measured distributions and extracted coefficients are compared with standard model predictions from simulations at next-to-leading-order (NLO) accuracy in quantum chromodynamics (QCD), and from NLO QCD calculations including electroweak corrections. All measurements are found to be consistent with the expectations of the standard model. The normalized differential cross sections are used in fits to constrain the anomalous chromomagnetic and chromoelectric dipole moments of the top quark to $-$0.24 $<C_\text{tG}/\Lambda^{2}$ $<$ 0.07 TeV$^{-2}$ and $-$0.33 $< C^{I}_\text{tG}/\Lambda^{2}$ $<$ 0.20 TeV$^{-2}$, respectively, at 95% confidence level.

29 data tables

Figure 4, normalized differential cross section for $\cos\theta_{1}^{k}$

Figure 4, normalized differential cross section for $\cos\theta_{2}^{k}$

Figure 4, normalized differential cross section for $\cos\theta_{1}^{r}$

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Measurement of the top quark mass in the all-jets final state at $\sqrt{s}=$ 13 TeV and combination with the lepton+jets channel

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
Eur.Phys.J.C 79 (2019) 313, 2019.
Inspire Record 1711672 DOI 10.17182/hepdata.89051

A top quark mass measurement is performed using 35.9 fb$^{-1}$ of LHC proton-proton collision data collected with the CMS detector at $\sqrt{s} =$ 13 TeV. The measurement uses the $\mathrm{t\overline{t}}$ all-jets final state. A kinematic fit is performed to reconstruct the decay of the $\mathrm{t\overline{t}}$ system and suppress the multijet background. Using the ideogram method, the top quark mass ($m_\mathrm{t}$) is determined, simultaneously constraining an additional jet energy scale factor (JSF). The resulting value of $m_\mathrm{t}$ = 172.34 $\pm$ 0.20 (stat+JSF) $\pm$ 0.70 (syst) GeV is in good agreement with previous measurements. In addition, a combined measurement that uses the $\mathrm{t\overline{t}}$ lepton+jets and all-jets final states is presented, using the same mass extraction method, and provides an $m_\mathrm{t}$ measurement of 172.26 $\pm$ 0.07 (stat+JSF) $\pm$ 0.61 (syst) GeV. This is the first combined $m_\mathrm{t}$ extraction from the lepton+jets and all-jets channels through a single likelihood function.

1 data table

Measured top quark mass $m_{t}$


Measurements of $\mathrm{t\overline{t}}$ differential cross sections in proton-proton collisions at $\sqrt{s} =$ 13 TeV using events containing two leptons

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
JHEP 02 (2019) 149, 2019.
Inspire Record 1703993 DOI 10.17182/hepdata.89307

Measurements of differential top quark pair $\mathrm{t\overline{t}}$ cross sections using events produced in proton-proton collisions at a centre-of-mass energy of 13 TeV containing two oppositely charged leptons are presented. The data were recorded by the CMS experiment at the CERN LHC in 2016 and correspond to an integrated luminosity of 35.9 fb$^{-1}$. The differential cross sections are presented as functions of kinematic observables of the top quarks and their decay products, the $\mathrm{t\overline{t}}$ system, and the total number of jets in the event. The differential cross sections are defined both with particle-level objects in a fiducial phase space close to that of the detector acceptance and with parton-level top quarks in the full phase space. All results are compared with standard model predictions from Monte Carlo simulations with next-to-leading-order (NLO) accuracy in quantum chromodynamics (QCD) at matrix-element level interfaced to parton-shower simulations. Where possible, parton-level results are compared to calculations with beyond-NLO precision in QCD. Significant disagreement is observed between data and all predictions for several observables. The measurements are used to constrain the top quark chromomagnetic dipole moment in an effective field theory framework at NLO in QCD and to extract $\mathrm{t\overline{t}}$ and leptonic charge asymmetries.

188 data tables

Measured absolute differential cross section at parton level as a function of $p_{T}^{t}$.

Covariance matrix of the absolute differential cross section at parton level as a function of $p_{T}^{t}$.

Measured normalised differential cross section at parton level as a function of $p_{T}^{t}$.

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Version 2
Measurement of jet substructure observables in $\mathrm{t\overline{t}}$ events from proton-proton collisions at $\sqrt{s} =$ 13TeV

The CMS collaboration Sirunyan, A. M. ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
Phys.Rev.D 98 (2018) 092014, 2018.
Inspire Record 1690148 DOI 10.17182/hepdata.84716

A measurement of jet substructure observables is presented using \ttbar events in the lepton+jets channel from proton-proton collisions at $\sqrt{s}=$ 13 TeV recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Multiple jet substructure observables are measured for jets identified as bottom, light-quark, and gluon jets, as well as for inclusive jets (no flavor information). The results are unfolded to the particle level and compared to next-to-leading-order predictions from POWHEG interfaced with the parton shower generators PYTHIA 8 and HERWIG 7, as well as from SHERPA 2 and DIRE2. A value of the strong coupling at the Z boson mass, $\alpha_S(m_\mathrm{Z}) = $ 0.115$^{+0.015}_{-0.013}$, is extracted from the substructure data at leading-order plus leading-log accuracy.

264 data tables

Distribution of $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.

Distribution of $\lambda_{0}^{0}$ (N) reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.

Distribution of $\lambda_{0}^{2}$ ($p_{T}^{d,*})$ reconstructed from charged particles with pt > 1 GeV, unfolded to the particle level.

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Measurement of the top quark mass with lepton+jets final states using pp collisions at $\sqrt{s}=$ 13 TeV

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
Eur.Phys.J.C 78 (2018) 891, 2018.
Inspire Record 1671499 DOI 10.17182/hepdata.85702

The mass of the top quark is measured using a sample of $\mathrm{t\overline{t}}$ events collected by the CMS detector using proton-proton collisions at $\sqrt{s} =$ 13 TeV at the CERN LHC. Events are selected with one isolated muon or electron and at least four jets from data corresponding to an integrated luminosity of 35.9 fb$^{-1}$. For each event the mass is reconstructed from a kinematic fit of the decay products to a $\mathrm{t\overline{t}}$ hypothesis. Using the ideogram method, the top quark mass is determined simultaneously with an overall jet energy scale factor (JSF), constrained by the mass of the W boson in $\mathrm{q\overline{q}'}$ decays. The measurement is calibrated on samples simulated at next-to-leading order matched to a leading-order parton shower. The top quark mass is found to be 172.25 $\pm$ 0.08 (stat+JSF) $\pm$ 0.62 (syst) GeV. The dependence of this result on the kinematic properties of the event is studied and compared to predictions of different models of $\mathrm{t\overline{t}}$ production, and no indications of a bias in the measurements are observed.

1 data table

Measured top quark mass $m_{t}$


Measurements of differential cross sections of top quark pair production in association with jets in ${pp}$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 10 (2018) 159, 2018.
Inspire Record 1656578 DOI 10.17182/hepdata.81950

Measurements of differential cross sections of top quark pair production in association with jets by the ATLAS experiment at the LHC are presented. The measurements are performed as functions of the top quark transverse momentum, the transverse momentum of the top quark-antitop quark system and the out-of-plane transverse momentum using data from $pp$ collisions at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC in 2015 and corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The top quark pair events are selected in the lepton (electron or muon) + jets channel. The measured cross sections, which are compared to several predictions, allow a detailed study of top quark production.

115 data tables

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration, obtained through the Bootstrap Method.

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and $p_{T}^{t,had}$ in the 4-jet exclusive configuration, obtained through the Bootstrap Method.

Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and $p_{T}^{t\bar{t}}$ in the 4-jet exclusive configuration, obtained through the Bootstrap Method.

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Measurement of the inclusive and fiducial $t\bar{t}$ production cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 78 (2018) 487, 2018.
Inspire Record 1644099 DOI 10.17182/hepdata.81945

The inclusive and fiducial $t\bar{t}$ production cross-sections are measured in the lepton+jets channel using 20.2 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of 8 TeV recorded with the ATLAS detector at the LHC. Major systematic uncertainties due to the modelling of the jet energy scale and $b$-tagging efficiency are constrained by separating selected events into three disjoint regions. In order to reduce systematic uncertainties in the most important background, the W+jets process is modelled using Z+jets events in a data-driven approach. The inclusive $t\bar{t}$ cross-section is measured with a precision of 5.7% to be $\sigma_{\text{inc}}(t\bar{t})$ = 248.3 $\pm$ 0.7 (stat.) $\pm$ 13.4 (syst.) $\pm$ 4.7 (lumi.) pb, assuming a top-quark mass of 172.5 GeV. The result is in agreement with the Standard Model prediction. The cross-section is also measured in a phase space close to that of the selected data. The fiducial cross-section is $\sigma_{\text{fid}}(t\bar{t})$ = 48.8 $\pm$ 0.1 (stat.) $\pm$ 2.0 (syst.) $\pm$ 0.9 (lumi.) pb with a precision of 4.5%.

2 data tables

The measured inclusive cross section. The first systematic uncertainty (sys_1) is the combined systematic uncertainty excluding luminosity, the second (sys_2) is the luminosity

The measured fiducial cross section. The first systematic uncertainty (sys_1) is the combined systematic uncertainty excluding luminosity, the second (sys_2) is the luminosity


Version 2
Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, M. ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 77 (2017) 804, 2017.
Inspire Record 1626105 DOI 10.17182/hepdata.77890

This paper presents single lepton and dilepton kinematic distributions measured in dileptonic $t\bar{t}$ events produced in 20.2 fb$^{-1}$ of $\sqrt{s}=8$ TeV $pp$ collisions recorded by the ATLAS experiment at the LHC. Both absolute and normalised differential cross-sections are measured, using events with an opposite-charge $e\mu$ pair and one or two $b$-tagged jets. The cross-sections are measured in a fiducial region corresponding to the detector acceptance for leptons, and are compared to the predictions from a variety of Monte Carlo event generators, as well as fixed-order QCD calculations, exploring the sensitivity of the cross-sections to the gluon parton distribution function. Some of the distributions are also sensitive to the top quark pole mass; a combined fit of NLO fixed-order predictions to all the measured distributions yields a top quark mass value of $m_t^{\rm pole}=173.2\pm 0.9\pm0.8\pm1.2$ GeV, where the three uncertainties arise from data statistics, experimental systematics, and theoretical sources.

32 data tables

Absolute differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

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Measurement of normalized differential t-tbar cross sections in the dilepton channel from pp collisions at sqrt(s) = 13 TeV

The CMS collaboration Sirunyan, A.M. ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
JHEP 04 (2018) 060, 2018.
Inspire Record 1620050 DOI 10.17182/hepdata.81686

Normalized differential cross sections for top quark pair production are measured in the dilepton (e$^+$e$^-$, $\mu^+\mu^-$, and $\mu^\mp$e$^\pm$) decay channels in proton-proton collisions at a center-of-mass energy of 13 TeV. The measurements are performed with data corresponding to an integrated luminosity of 2.1 fb$^{-1}$ using the CMS detector at the LHC. The cross sections are measured differentially as a function of the kinematic properties of the leptons, jets from bottom quark hadronization, top quarks, and top quark pairs at the particle and parton levels. The results are compared to several Monte Carlo generators that implement calculations up to next-to-leading order in perturbative quantum chromodynamics interfaced with parton showering, and also to fixed-order theoretical calculations of top quark pair production up to next-to-next-to-leading order.

28 data tables

Normalized differential ttbar cross sections with statistical and systematic uncertainties at the particle level as a function of pt(lepton).

Normalized differential ttbar cross sections with statistical and systematic uncertainties at the particle level as a function of pt(jet).

Normalized differential ttbar cross sections with statistical and systematic uncertainties at the particle level as a function of pt(top).

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Version 2
Measurements of top-quark pair differential cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s}$=13 TeV using the ATLAS detector

The ATLAS collaboration Aaboud, M. ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 11 (2017) 191, 2017.
Inspire Record 1614149 DOI 10.17182/hepdata.80041

Measurements of differential cross-sections of top-quark pair production in fiducial phase-spaces are presented as a function of top-quark and $t\bar{t}$ system kinematic observables in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$=13 TeV. The data set corresponds to an integrated luminosity of $3.2$ fb${}^{-1}$, recorded in 2015 with the ATLAS detector at the CERN Large Hadron Collider. Events with exactly one electron or muon and at least two jets in the final state are used for the measurement. Two separate selections are applied that each focus on different top-quark momentum regions, referred to as resolved and boosted topologies of the $t\bar{t}$ final state. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ and $p$-values.

56 data tables

Covariance matrix of the absolute cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the absolute cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.

Covariance matrix of the relative cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.

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Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions

The CMS collaboration Sirunyan, Albert M ; Tumasyan, Armen ; Adam, Wolfgang ; et al.
Eur.Phys.J.C 77 (2017) 459, 2017.
Inspire Record 1516191 DOI 10.17182/hepdata.77008

Normalized double-differential cross sections for top quark pair (t t-bar) production are measured in pp collisions at a centre-of-mass energy of 8 TeV with the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 19.7 inverse femtobarns. The measurement is performed in the dilepton e+/- mu-/+ final state. The t t-bar cross section is determined as a function of various pairs of observables characterizing the kinematics of the top quark and t t-bar system. The data are compared to calculations using perturbative quantum chromodynamics at next-to-leading and approximate next-to-next-to-leading orders. They are also compared to predictions of Monte Carlo event generators that complement fixed-order computations with parton showers, hadronization, and multiple-parton interactions. Overall agreement is observed with the predictions, which is improved when the latest global sets of proton parton distribution functions are used. The inclusion of the measured t t-bar cross sections in a fit of parametrized parton distribution functions is shown to have significant impact on the gluon distribution.

18 data tables

The measured normalized $t\bar{t}$ double-differential cross sections in different bins of $y(t)$ and $p_{T}(t)$, along with their relative statistical and systematic uncertainties expressed as percentages.

The correlation matrix of statistical uncertainties for the normalized $t\bar{t}$ double-differential cross sections as a function of $y(t)$ and $p_{T}(t)$. The values are expressed as percentages. For bin indices see Table 5.

Sources and values of the relative systematic uncertainties in percent of the measured normalized $t\bar{t}$ double-differential cross sections as a function of $y(t)$ and $p_{T}(t)$. For bin indices see Table 5.

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Measurements of top-quark pair to $Z$-boson cross-section ratios at $\sqrt s = 13, 8, 7$TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 02 (2017) 117, 2017.
Inspire Record 1502921 DOI 10.17182/hepdata.75536

Ratios of top-quark pair to $Z$-boson cross sections measured from proton--proton collisions at the LHC centre-of-mass energies of $\sqrt s=13$TeV, 8TeV, and 7TeV are presented by the ATLAS Collaboration. Single ratios, at a given $\sqrt s$ for the two processes and at different $\sqrt s$ for each process, as well as double ratios of the two processes at different $\sqrt s$, are evaluated. The ratios are constructed using previously published ATLAS measurements of the $t\overline{t}$ and $Z$-boson production cross sections, corrected to a common phase space where required, and a new analysis of $Z \rightarrow \ell^+ \ell^-$ where $\ell=e,\mu$ at $\sqrt s=13$TeV performed with data collected in 2015 with an integrated luminosity of $3.2$fb$^{-1}$. Correlations of systematic uncertainties are taken into account when evaluating the uncertainties in the ratios. The correlation model is also used to evaluate the combined cross section of the $Z\rightarrow e^+e^-$ and the $Z\rightarrow \mu^+ \mu^-$ channels for each $\sqrt s$ value. The results are compared to calculations performed at next-to-next-to-leading-order accuracy using recent sets of parton distribution functions. The data demonstrate significant power to constrain the gluon distribution function for the Bjorken-$x$ values near 0.1 and the light-quark sea for $x<0.02$.

11 data tables

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+e- final state at 13TeV.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state at 13TeV.

Breakdown of systematic uncertainties in percent for the measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+e- final state at 13TeV.

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Measurement of the ttbbar production cross section using events in the e mu final state in pp collisions at sqrt(s)=13 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Eur.Phys.J.C 77 (2017) 172, 2017.
Inspire Record 1497736 DOI 10.17182/hepdata.76735

The cross section of top quark-antiquark pair production in proton-proton collisions at sqrt(s) = 13 TeV is measured by the CMS experiment at the LHC, using data corresponding to an integrated luminosity of 2.2 inverse femtobarns. The measurement is performed by analyzing events in which the final state includes one electron, one muon, and two or more jets, at least one of which is identified as originating from hadronization of a b quark. The measured cross section is 815 +/- 9 (stat) +/- 38 (syst) +/- 19 (lumi) pb, in agreement with the expectation from the standard model.

3 data tables

Summary of the individual contributions to the uncertainty in the $\sigma_{t\bar{t}}$ measurement.

Measurement of the $t\bar{t}$ production cross-section in $pp$ collisions at $\sqrt{s} = 13$ TeV.

Number of dilepton events obtained after applying the full selection. The results are given for the individual sources of background, $t\bar{t}$ signal with a top quark mass of 172.5 GeV and $\sigma_{t\bar{t}}$ = 832 +/- 46 pb, and data. The uncertainties correspond to statistical and systematic components.


Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 95 (2017) 092001, 2017.
Inspire Record 1491950 DOI 10.17182/hepdata.76554

Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3 inverse femtobarns. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.

164 data tables

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

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Measurement of the mass of the top quark in decays with a J/psi meson in pp collisions at 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
JHEP 12 (2016) 123, 2016.
Inspire Record 1480862 DOI 10.17182/hepdata.75539

A first measurement of the top quark mass using the decay channel t to (W to l nu) (b to J/psi + X to mu+ mu- + X) is presented. The analysis uses events selected from the proton-proton collisions recorded with the CMS detector at the LHC at a center-of-mass energy of 8 TeV. The data correspond to an integrated luminosity of 19.7 inverse femtobarns, with 666 t t-bar and single top quark candidate events containing a reconstructed J/psi candidate decaying into an oppositely-charged muon pair. The mass of the (J/psi + l) system, where l is an electron or a muon from W boson decay, is used to extract a top quark mass of 173.5 +/- 3.0 (stat) +/- 0.9 (syst) GeV.

2 data tables

Number of selected events from simulations and observed in data. The uncertainties are statistical.

Summary of the impact of systematic uncertainties on the top quark mass according to the contributions from each source.


Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Rev.D 94 (2016) 092003, 2016.
Inspire Record 1477814 DOI 10.17182/hepdata.75323

Measurements of normalized differential cross-sections of top quark pair ($t\bar t$) production are presented as a function of the mass, the transverse momentum and the rapidity of the $t\bar t$ system in proton-proton collisions at center-of-mass energies of $\sqrt{s}$ = 7 TeV and 8 TeV. The dataset corresponds to an integrated luminosity of 4.6 fb$^{-1}$ at 7 TeV and 20.2 fb$^{-1}$ at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a $b$-hadron. The measured distributions are corrected for detector effects and selection efficiency to cross-sections at the parton level. The differential cross-sections are compared with different Monte Carlo generators and theoretical calculations of $t\bar t$ production. The results are consistent with the majority of predictions in a wide kinematic range.

36 data tables

Parton-level normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.

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Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at sqrt(s) = 7 and 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 94 (2016) 052006, 2016.
Inspire Record 1473674 DOI 10.17182/hepdata.74124

Measurements are reported of the normalized differential cross sections for top quark pair production with respect to four kinematic event variables: the missing transverse energy; the scalar sum of the jet transverse momentum (pT); the scalar sum of the pT of all objects in the event; and the pT of leptonically decaying W bosons from top quark decays. The data sample, collected using the CMS detector at the LHC, consists of 5.0 inverse femtobarns of proton-proton collisions at sqrt(s) = 7 TeV and 19.7 inverse femtobarns at sqrt(s) = 8 TeV. Top quark pair events containing one electron or muon are selected. The results are presented after correcting for detector effects to allow direct comparison with theoretical predictions. No significant deviations from the predictions of several standard model event simulation generators are observed.

16 data tables

Normalized $t\bar{t}$ differential cross section measurements with respect to the $E^{miss}_{T}$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).

Normalized $t\bar{t}$ differential cross section measurements with respect to the $H_T$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).

Normalized $t\bar{t}$ differential cross section measurements with respect to the $S_T$ variable at a center-of-mass energy of 7 TeV (combination of electron and muon channels).

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Measurement of the $t\bar{t}$ production cross-section using $e\mu$ events with b-tagged jets in pp collisions at $\sqrt{s}$=13 TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 761 (2016) 136-157, 2016.
Inspire Record 1468168 DOI 10.17182/hepdata.73120

This paper describes a measurement of the inclusive top quark pair production cross-section ($\sigma_{t\bar{t}}$) with a data sample of 3.2 fb$^{-1}$ of proton--proton collisions at a centre-of-mass energy of $\sqrt{s}$=13 TeV, collected in 2015 by the ATLAS detector at the LHC. This measurement uses events with an opposite-charge electron--muon pair in the final state. Jets containing $b$-quarks are tagged using an algorithm based on track impact parameters and reconstructed secondary vertices. The numbers of events with exactly one and exactly two $b$-tagged jets are counted and used to determine simultaneously $\sigma_{t\bar{t}}$ and the efficiency to reconstruct and $b$-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section is measured to be: $\sigma_{t\bar{t}}$= 818 $\pm$ 8 (stat) $\pm$ 27 (syst) $\pm$ 19 (lumi) $\pm$ 12 (beam) pb, where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, the integrated luminosity and the LHC beam energy, giving a total relative uncertainty of 4.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. A fiducial measurement corresponding to the experimental acceptance of the leptons is also presented.

2 data tables

Measured cross-section for $t\bar{t}$ events using $e\mu$ events with b-tagged jets in pp collisions at $\sqrt{s}$=13 TeV.

Measured fiducial cross-section for $t\bar{t}$ events producing an $e\mu$ pair, each lepton originating directly from t $\rightarrow$ W $\rightarrow$ l or via a leptonic $\tau$ decay t $\rightarrow$ W $\rightarrow$ $\tau$ $\rightarrow$ l and satisfying p$_{\mathrm{T}} > $ 25 GeV and $|\eta| <$ 2.5.


Measurement of the W boson helicity fractions in the decays of top quark pairs to lepton+jets final states produced in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Lett.B 762 (2016) 512-534, 2016.
Inspire Record 1466294 DOI 10.17182/hepdata.74337

The W boson helicity fractions from top quark decays in t t-bar events are measured using data from proton-proton collisions at a centre-of-mass energy of 8 TeV. The data were collected in 2012 with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.8 inverse femtobarns. Events are reconstructed with either one muon or one electron, along with four jets in the final state, with two of the jets being identified as originating from b quarks. The measured helicity fractions from both channels are combined, yielding F[0] = 0.681 +/- 0.012 (stat) +/- 0.023 (syst), F[L] = 0.323 +/- 0.008 (stat) +/- 0.014 (syst), and F[R] = -0.004 +/- 0.005 (stat) +/- 0.014 (syst) for the longitudinal, left-, and right-handed components of the helicity, respectively. These measurements of the W boson helicity fractions are the most accurate to date and they agree with the predictions from the standard model.

3 data tables

Measurement of the W longitudinal (F0), left- (FL) and righ- (FR) components of the boson helicity fractions from electron+jets final states in top quark pair decays. The helicity fractions F0 and FL are measured simultaneously and are strongly anti-correlated, with statistical correlation coefficient -0.950.

Measurement of the W longitudinal (F0), left- (FL) and righ- (FR) components of the boson helicity fractions from muon+jets final states in top quark pair decays. The helicity fractions F0 and FL are measured simultaneously and are strongly anti-correlated, with statistical correlation coefficient -0.957.

Measurement of the W longitudinal (F0), left- (FL) and righ- (FR) components of the boson helicity fractions from lepton+jets final states in top quark pair decays. The helicity fractions F0 and FL are measured simultaneously and are strongly anti-correlated, with statistical correlation coefficient -0.959, and total correlation, considering both statistical and systematic uncertainties, of -0.87.


Measurement of the integrated and differential t-tbar production cross sections for high-pt top quarks in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 94 (2016) 072002, 2016.
Inspire Record 1454211 DOI 10.17182/hepdata.78540

The cross section for pair production of top quarks (t-tbar) with high transverse momenta is measured in pp collisions, collected with the CMS detector at the LHC with sqrt(s) = 8 TeV in data corresponding to an integrated luminosity of 19.7 inverse femtobarns. The measurement is performed using lepton+jets events, where one top quark decays semileptonically, while the second top quark decays to a hadronic final state. The hadronic decay is reconstructed as a single, large-radius jet, and identified as a top quark candidate using jet substructure techniques. The integrated cross section and the differential cross sections as a function of top quark pt and rapidity are measured at particle level within a fiducial region related to the detector-level requirements and at parton level. The particle-level integrated cross section is found to be sigma[t-tbar] = 0.499 +/- 0.035 (stat+syst) +/- 0.095 (theory) +/- 0.013 (lumi) pb for top quark pt > 400 GeV. The parton-level measurement is sigma[t-tbar] = 1.44 +/- 0.10 (stat+syst) +/- 0.29 (theory) +/- 0.04 (lumi) pb. The integrated and differential cross section results are compared to predictions from several event generators.

3 data tables

The measurements of the integrated cross sections for $p_T^t > 400$ GeV.

Differential $t\bar{t}$ cross section in bins of $p_T$ for the $t$ jet at the particle level and the top quark at parton level.

Differential $t\bar{t}$ cross section in bins of $y$ for the $t$ jet at the particle level and the top quark at parton level.


Measurement of the top quark mass using charged particles in collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 93 (2016) 092006, 2016.
Inspire Record 1430902 DOI 10.17182/hepdata.72898

A novel technique for measuring the mass of the top quark that uses only the kinematic properties of its charged decay products is presented. Top quark pair events with final states with one or two charged leptons and hadronic jets are selected from the data set of 8 TeV proton-proton collisions, corresponding to an integrated luminosity of 19.7 inverse femtobarns. By reconstructing secondary vertices inside the selected jets and computing the invariant mass of the system formed by the secondary vertex and an isolated lepton, an observable is constructed that is sensitive to the top quark mass that is expected to be robust against the energy scale of hadronic jets. The main theoretical systematic uncertainties, concerning the modeling of the fragmentation and hadronization of b quarks and the reconstruction of secondary vertices from the decays of b hadrons, are studied. A top quark mass of 173.68 +/- 0.20 (stat) +1.58 -0.97 (syst) GeV is measured. The overall systematic uncertainty is dominated by the uncertainty in the b quark fragmentation and the modeling of kinematic properties of the top quark.

3 data tables

Combined measurement of the top quark mass.

Number of observed events and expected purity of top quark production ($t\bar{t}$ and single top quarks) for the five channels investigated in this analysis.

Summary of the systematic uncertainties in the final measurement. In cases where there are two variations of one source of uncertainty, the first and second numbers correspond, respectively, to the down and up variations. The total uncertainties are taken as the separate quadratic sum of all positive and negative shifts. For the contributions marked with a (*), the shift of the single variation including its sign is given, but the uncertainty is counted symmetrically in both up and down directions for the total uncertainty calculation.


Measurements of t t-bar charge asymmetry using dilepton final states in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Lett.B 760 (2016) 365-386, 2016.
Inspire Record 1430892 DOI 10.17182/hepdata.71444

The charge asymmetry in t t-bar events is measured using dilepton final states produced in pp collisions at the LHC at sqrt(s) = 8 TeV. The data sample, collected with the CMS detector, corresponds to an integrated luminosity of 19.5 inverse femtobarns. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The charge asymmetry is measured from differences in kinematic distributions, unfolded to the parton level, of positively and negatively charged top quarks and leptons. The t t-bar and leptonic charge asymmetries are found to be 0.011 +/- 0.011 (stat) +/- 0.007 (syst) and 0.003 +/- 0.006 (stat) +/- 0.003 (syst), respectively. These results, as well as charge asymmetry measurements made as a function of the invariant mass, rapidity, and transverse momentum of the t t-bar system, are in agreement with predictions of the standard model.

43 data tables

Inclusive values of the asymmetry variables.

Values of the 6 bins of the normalized differential cross section as a function of $\Delta|y_\mathrm{t}|$.

Statistical covariance matrix for the 6 bins of the normalized differential cross section as a function of $\Delta|y_\mathrm{t}|$.

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Measurement of the t-tbar production cross section in the e-mu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
JHEP 08 (2016) 029, 2016.
Inspire Record 1426692 DOI 10.17182/hepdata.74208

The inclusive cross section for top quark pair production is measured in proton-proton collisions at sqrt(s) = 7 and 8 TeV, corresponding to 5.0 and 19.7 invers-femtobarns, respectively, with the CMS experiment at the LHC. The cross sections are measured in the electron-muon channel using a binned likelihood fit to multi-differential final state distributions related to identified b quark jets and other jets in the event. The measured cross section values are 173.6 +/- 2.1 (stat) +4.5-4.0 (syst) +/- 3.8 (lumi) pb at sqrt(s) = 7 TeV, and 244.9 +/- 1.4 (stat) +6.3-5.5 (syst) +/- 6.4 (lumi) pb at sqrt(s) = 8 TeV, in good agreement with QCD calculations at next-to-next-to-leading-order accuracy. The ratio of the cross sections measured at 7 and 8 TeV is determined, as well as cross sections in the fiducial regions defined by the acceptance requirements on the two charged leptons in the final state. The cross section results are used to determine the top quark pole mass via the dependence of the theoretically predicted cross section on the mass, giving a best result of 173.8 +1.7-1.8 GeV. The data at sqrt(s) = 8 TeV are also used to set limits, for two neutralino mass values, on the pair production of supersymmetric top squarks with masses close to the top quark mass.

3 data tables

Measurement of the visible $t\bar{t}$ production cross-section in $pp$ collisions at $\sqrt{s} = 7$ and $8$ TeV. The visible cross section is defined for events containing an oppositely charged $\rm{e}\mu$ pair from the decay chain ${\rm t} \rightarrow {\rm W b} \rightarrow {\ell} \nu {\rm b}$ (including ${\rm W} \rightarrow \tau \nu \rightarrow {\ell} \nu \nu \nu$) and with both leptons satisfying $p_T > 20\, \rm{GeV}$ and $|{\eta}| < 2.4$.

Measurement of the inclusive $t\bar{t}$ production cross-section in $pp$ collisions at $\sqrt{s} = 7$ and $8$ TeV.

Top quark pole mass at NNLO+NNLL extracted by comparing the measured $t\bar{t}$ production cross sections at 7 and 8 TeV with predictions employing different PDF sets. The uncertainties of the CT14 PDF set are scaled to 68% confidence level.


Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, V. ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 93 (2016) 052007, 2016.
Inspire Record 1413748 DOI 10.17182/hepdata.70879

Measurements of the top quark-antiquark (t t-bar) spin correlations and the top quark polarization are presented for t t-bar pairs produced in pp collisions at sqrt(s) = 8 TeV. The data correspond to an integrated luminosity of 19.5 inverse femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the t t-bar system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

106 data tables

Inclusive values of the asymmetry variables.

Values of the 12 bins of the normalized differential cross section as a function of $\left|\Delta \phi_{\ell^+\ell^-}\right|$.

Statistical covariance matrix for the 12 bins of the normalized differential cross section as a function of $\left|\Delta \phi_{\ell^+\ell^-}\right|$.

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Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Lett.B 756 (2016) 52-71, 2016.
Inspire Record 1410588 DOI 10.17182/hepdata.77021

In the $pp \rightarrow t\bar{t}$ process the angular distributions of top and anti-top quarks are expected to present a subtle difference, which could be enhanced by processes not included in the Standard Model. This Letter presents a measurement of the charge asymmetry in events where the top-quark pair is produced with a large invariant mass. The analysis is performed on 20.3 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} =$ 8 TeV collected by the ATLAS experiment at the LHC, using reconstruction techniques specifically designed for the decay topology of highly boosted top quarks. The charge asymmetry in a fiducial region with large invariant mass of the top-quark pair ($m_{t\bar{t}} > $ 0.75 TeV) and an absolute rapidity difference of the top and anti-top quark candidates within $-$2 $ < |y_t| - |y_{\bar{t}}| <$ 2 is measured to be 4.2 $\pm$ 3.2%, in agreement with the Standard Model prediction at next-to-leading order. A differential measurement in three $t\bar{t}$ mass bins is also presented.

1 data table

The measured charge asymmetry after the unfolding to parton level in four intervals of the invariant mass of the $t\bar{t}$ system. The phase space is limited to $|(\Delta |y|)|<$ 2. The uncertainties correspond to the sum in quadrature of statistical and systematic uncertainties (for the data) or to the theory uncertainty (for the SM prediction).


Measurement of spin correlations in t t-bar production using the matrix element method in the muon + jets final state in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Lett.B 758 (2016) 321-346, 2016.
Inspire Record 1405439 DOI 10.17182/hepdata.70230

The consistency of the spin correlation strength in top quark pair production with the standard model (SM) prediction is tested in the muon + jets final state. The events are selected from pp collisions, collected by the CMS detector, at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.7 inverse femtobarns. The data are compared with the expectation for the spin correlation predicted by the SM and with the expectation of no correlation. Using a template fit method, the fraction of events that show SM spin correlations is measured to be 0.72 +/- 0.08 (stat) +0.15 -0.13 (syst), representing the most precise measurement of this quantity in the lepton + jets final state to date.

1 data table

The result of the template fit of distributions for uncorrelated and SM-like correlated ttbar spins.


Version 2
Measurements of top-quark pair differential cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Eur.Phys.J.C 76 (2016) 538, 2016.
Inspire Record 1404878 DOI 10.17182/hepdata.84154

Measurements of normalized differential cross-sections of top-quark pair production are presented as a function of the top-quark, $t\bar{t}$ system and event-level kinematic observables in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=8$ TeV}. The observables have been chosen to emphasize the $t\bar{t}$ production process and to be sensitive to effects of initial- and final-state radiation, to the different parton distribution functions, and to non-resonant processes and higher-order corrections. The dataset corresponds to an integrated luminosity of 20.3 fb$^{-1}$, recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of the jets tagged as originating from a $b$-quark. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations. The results are in fair agreement with the predictions over a wide kinematic range. Nevertheless, most generators predict a harder top-quark transverse momentum distribution at high values than what is observed in the data. Predictions beyond NLO accuracy improve the agreement with data at high top-quark transverse momenta. Using the current settings and parton distribution functions, the rapidity distributions are not well modelled by any generator under consideration. However, the level of agreement is improved when more recent sets of parton distribution functions are used.

236 data tables

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.

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Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV using the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Rev.D 93 (2016) 012002, 2016.
Inspire Record 1400803 DOI 10.17182/hepdata.76911

A measurement of the correlations between the polar angles of leptons from the decay of pair-produced $t$ and $\bar{t}$ quarks in the helicity basis is reported, using proton-proton collision data collected by the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 4.6fb$^{-1}$ at a center-of-mass energy of $\sqrt{s}=7$TeV collected during 2011. Candidate events are selected in the dilepton topology with large missing transverse momentum and at least two jets. The angles $\theta_1$ and $\theta_2$ between the charged leptons and the direction of motion of the parent quarks in the $t\bar{t}$ rest frame are sensitive to the spin information, and the distribution of {\mbox{$\cos\theta_1\cdot\cos\theta_2$}} is sensitive to the spin correlation between the $t$ and $\bar{t}$ quarks. The distribution is unfolded to parton level and compared to the next-to-leading order prediction. A good agreement is observed.

2 data tables

The numerical summary of the unfolded $\cos\theta_1\cdot\cos\theta_2$ distribution, with statistical and systematic uncertainties.

The correlation factors for the statistical uncertainties between any two bins of the unfolded distribution.


Measurement of the top quark pair production cross section in proton-proton collisions at sqrt(s)=13 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.Lett. 116 (2016) 052002, 2016.
Inspire Record 1398582 DOI 10.17182/hepdata.69538

The top quark pair production cross section is measured for the first time in proton-proton collisions at sqrt(s) = 13 TeV by the CMS experiment at the CERN LHC, using data corresponding to an integrated luminosity of 43 inverse picobarns. The measurement is performed by analyzing events with at least one electron and one muon of opposite charge, and at least two jets. The measured cross section is 746 +/- 58 (stat) +/- 53 (syst) +/- 36 (lumi) pb, in agreement with the expectation from the standard model.

1 data table

The first measurement of the $t\bar{t}$ production cross-section in $pp$ collisions at $\sqrt{s} = 13$ TeV.


Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in $\sqrt{s}$ = 8 TeV proton-proton collisions using the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Rev.D 93 (2016) 032009, 2016.
Inspire Record 1397637 DOI 10.17182/hepdata.18108

The differential cross-section for pair production of top quarks with high transverse momentum is measured in 20.3 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 8 TeV. The measurement is performed for $t\bar{t}$ events in the lepton+jets channel. The cross-section is reported as a function of the hadronically decaying top quark transverse momentum for values above 300 GeV. The hadronically decaying top quark is reconstructed as an anti-$k_t$ jet with radius parameter $R=1.0$ and identified with jet substructure techniques. The observed yield is corrected for detector effects to obtain a cross-section at particle level in a fiducial region close to the event selection. A parton-level cross-section extrapolated to the full phase space is also reported for top quarks with transverse momentum above 300 GeV. The predictions of a majority of next-to-leading-order and leading-order matrix-element Monte Carlo generators are found to agree with the measured cross-sections.

10 data tables

Fiducial particle-level differential cross-section, with statistical and systematic uncertainties, as a function of the top-jet candidate p_T.

Parton-level differential cross-section, with statistical and systematic uncertainties, as a function of the hadronically decaying top quark p_T.

The individual systematic uncertainties calculated as a percentage of the particle-level differential cross-section $d\sigma_{tt} / d p_{T,ptcl}$ in each bin. Variations on the two sides ("UP" and "DOWN") are separately quoted with their respective signs. Uncertainties smaller than 0.1% are neglected.

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Measurement of t-tbar production with additional jet activity, including b quark jets, in the dilepton channel using pp collisions at sqrt(s) = 8TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Eur.Phys.J.C 76 (2016) 379, 2016.
Inspire Record 1397174 DOI 10.17182/hepdata.70880

Jet multiplicity distributions in top quark pair (t t-bar) events are measured in pp collisions at a centre-of-mass energy of 8 TeV with the CMS detector at the LHC using a data set corresponding to an integrated luminosity of 19.7 inverse femtobarns. The measurement is performed in the dilepton decay channels (e+ e-, mu+ mu-, and e+/- mu-/+). The absolute and normalized differential cross sections for t t-bar production are measured as a function of the jet multiplicity in the event for different jet transverse momentum thresholds and the kinematic properties of the leading additional jets. The differential t t-bar b and t t-bar b b-bar cross sections are presented for the first time as a function of the kinematic properties of the leading additional b jets. Furthermore, the fraction of events without additional jets above a threshold is measured as a function of the transverse momenta of the leading additional jets and the scalar sum of the transverse momenta of all additional jets. The data are compared and found to be consistent with predictions from several perturbative quantum chromodynamics event generators and a next-to-leading order calculation.

76 data tables

Absolute differential ttbar cross sections as a function of the jet multiplicity for jets with pt > 30GeV, along with their statistical and systematic uncertainties. The results are presented at the particle level in the visible phase space of the ttbar decay products and the additional jets.

Normalized differential ttbar cross sections as a function of the jet multiplicity for jets with pt > 30GeV, along with their statistical and systematic uncertainties. The results are presented at the particle level in the visible phase space of the ttbar decay products and the additional jets.

Absolute differential ttbar cross sections as a function of the jet multiplicity for jets with pt > 60GeV, along with their statistical and systematic uncertainties. The results are presented at the particle level in the visible phase space of the ttbar decay products and the additional jets.

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Measurement of the top quark mass using proton-proton data at ${\sqrt{(s)}}$ = 7 and 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 93 (2016) 072004, 2016.
Inspire Record 1393269 DOI 10.17182/hepdata.71988

A new set of measurements of the top quark mass are presented, based on the proton-proton data recorded by the CMS experiment at the LHC at sqrt(s) = 8 TeV corresponding to a luminosity of 19.7 inverse femtobarns. The top quark mass is measured using the lepton + jets, all-jets and dilepton decay channels, giving values of 172.35 +/- 0.16 (stat) +/- 0.48 (syst) GeV, 172.32 +/- 0.25 (stat) +/- 0.59 (syst) GeV, and 172.82 +/- 0.19 (stat) +/- 1.22 (syst) GeV, respectively. When combined with the published CMS results at sqrt(s) = 7 TeV, they provide a top quark mass measurement of 172.44 +/- 0.13 (stat) +/- 0.47 (syst) GeV. The top quark mass is also studied as a function of the event kinematical properties in the lepton + jets decay channel. No indications of a kinematic bias are observed and the collision data are consistent with a range of predictions from current theoretical models of t t-bar production.

9 data tables

Measurement of $m_{t}$ as a function of the transverse momentum of the hadronically decaying top quark.

Measurement of $m_{t}$ as a function of the invariant mass of the tt¯ system.

Measurement of $m_{t}$ as a function of the transverse momentum of the tt¯ system.

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Measurement of the charge asymmetry in top-quark pair production in the lepton-plus-jets final state in $pp$ collision data at $\sqrt{s}=8$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Eur.Phys.J.C 76 (2016) 87, 2016.
Inspire Record 1392455 DOI 10.17182/hepdata.75528

This paper reports inclusive and differential measurements of the $t\bar{t}$ charge asymmetry $A_{\textrm{C}}$ in 20.3 fb$^{-1}$ of $\sqrt{s} = 8$ TeV $pp$ collisions recorded by the ATLAS experiment at the Large Hadron Collider at CERN. Three differential measurements are performed as a function of the invariant mass, transverse momentum and longitudinal boost of the $t\bar{t}$ system. The $t\bar{t}$ pairs are selected in the single-lepton channels ($e$ or $\mu$) with at least four jets, and a likelihood fit is used to reconstruct the $t\bar{t}$ event kinematics. A Bayesian unfolding procedure is performed to infer the asymmetry at parton level from the observed data distribution. The inclusive $t\bar{t}$ charge asymmetry is measured to be $A_{\textrm{C}} = 0.009 \pm 0.005$ (stat.$+$syst.). The inclusive and differential measurements are compatible with the values predicted by the Standard Model.

7 data tables

The inclusive $t\bar{t}$ production charge asymmetry, $A_C$, with statistical and systematic uncertainties combined.

Measured charge asymmetry, $A_C$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ invariant mass, $m_{t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.

Measured charge asymmetry, $A_C$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ velocity along the z-axis, $\beta_{z,t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.

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Measurement of the charge asymmetry in top quark pair production in pp collisions at sqrt(s) = 8 TeV using a template method

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Rev.D 93 (2016) 034014, 2016.
Inspire Record 1388178 DOI 10.17182/hepdata.69208

The charge asymmetry in the production of top quark and antiquark pairs is measured in proton-proton collisions at a center-of-mass energy of 8 TeV. The data, corresponding to an integrated luminosity of 19.6 inverse femtobarns, were collected by the CMS experiment at the LHC. Events with a single isolated electron or muon, and four or more jets, at least one of which is likely to have originated from hadronization of a bottom quark, are selected. A template technique is used to measure the asymmetry in the distribution of differences in the top quark and antiquark absolute rapidities. The measured asymmetry is A[c,y] = [0.33 +/- 0.26 (stat) +/- 0.33 (syst)]%, which is the most precise result to date. The results are compared to calculations based on the standard model and on several beyond-the-standard-model scenarios.

1 data table

The measured $t\bar{t}$ production asymmetry $A_c^y$.


Inclusive and differential measurements of the t t-bar charge asymmetry in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Phys.Lett.B 757 (2016) 154-179, 2016.
Inspire Record 1382590 DOI 10.17182/hepdata.68759

The t t-bar charge asymmetry is measured in proton-proton collisions at a centre-of-mass energy of 8 TeV. The data, collected with the CMS experiment at the LHC, correspond to an integrated luminosity of 19.7 inverse femtobarns. Selected events contain an electron or a muon and four or more jets, where at least one jet is identified as originating from b-quark hadronization. The inclusive charge asymmetry is found to be 0.0010 +/- 0.0068 (stat) +/- 0.0037 (syst). In addition, differential charge asymmetries as a function of rapidity, transverse momentum, and invariant mass of the t t-bar system are studied. For the first time at the LHC, the measurements are also performed in a reduced fiducial phase space of top quark pair production, with an integrated result of -0.0035 +/- 0.0072 (stat) +/- 0.0031 (syst). All measurements are consistent within two standard deviations with zero asymmetry as well as with the predictions of the standard model.

16 data tables

Corrected asymmetry as a function of $|y_\mathrm{t\bar{t}}|$ in the fiducial phase space. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.

Correlation matrix for the asymmetries as a function of $|y_\mathrm{t\bar{t}}|$ in the fiducial phase space. Both statistical and systematic effects are considered.

Corrected asymmetry as a function of $p_\text{T}^\mathrm{t\bar{t}}$ in the fiducial phase space. The value 9999 is used as a placeholder for infinity. The correlation matrix for these values can be found in a separate table.

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Measurement of colour flow with the jet pull angle in $t\bar{t}$ events using the ATLAS detector at $\sqrt{s}=8$ TeV

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Lett.B 750 (2015) 475-493, 2015.
Inspire Record 1376945 DOI 10.17182/hepdata.71235

The distribution and orientation of energy inside jets is predicted to be an experimental handle on colour connections between the hard--scatter quarks and gluons initiating the jets. This Letter presents a measurement of the distribution of one such variable, the jet pull angle. The pull angle is measured for jets produced in $t\bar{t}$ events with one $W$ boson decaying leptonically and the other decaying to jets using 20.3 fb$^{-1}$ of data recorded with the ATLAS detector at a centre-of-mass energy of $\sqrt{s}=8$ TeV at the LHC. The jet pull angle distribution is corrected for detector resolution and acceptance effects and is compared to various models.

6 data tables

Normalised fiducial ttbar differential cross-section for the jet pull angle distribution constructed using all particles.

Normalised fiducial ttbar differential cross-section for the jet pull angle distribution constructed using charged particles.

Statistical bin-bin correlation matrix.

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A search for $t\bar{t}$ resonances using lepton-plus-jets events in proton-proton collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 08 (2015) 148, 2015.
Inspire Record 1373299 DOI 10.17182/hepdata.70548

A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb$^{-1}$ of proton-proton collision data collected at a centre-of-mass energy of $\sqrt{s}=8$ TeV. The lepton-plus-jets final state is used, where the top pair decays to $W^+bW^-\bar{b}$, with one $W$ boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow $Z'$ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour $Z'$ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with $\Gamma/m =$ 15% decaying to $t\bar{t}$. These range from 2.5 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.

16 data tables

Selection efficiency x Acceptance for a Z' resonance.

Selection efficiency x Acceptance for a KK gluon resonance.

Selection efficiency x Acceptance for a KK graviton resonance.

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Measurement of the differential cross section for top quark pair production in pp collisions at sqrt(s) = 8 TeV

The CMS collaboration Khachatryan, Vardan ; Sirunyan, Albert M ; Tumasyan, Armen ; et al.
Eur.Phys.J.C 75 (2015) 542, 2015.
Inspire Record 1370682 DOI 10.17182/hepdata.68516

The normalized differential cross section for top quark pair (tt-bar) production is measured in pp collisions at a centre-of-mass energy of 8 TeV at the CERN LHC using the CMS detector in data corresponding to an integrated luminosity of 19.7 inverse femtobarns. The measurements are performed in the lepton + jets (e/mu + jets) and in the dilepton (e+e-, mu+mu-, and e+-mu-+) decay channels. The tt-bar cross section is measured as a function of the kinematic properties of the charged leptons, the jets associated to b quarks, the top quarks, and the tt-bar system. The data are compared with several predictions from perturbative quantum chromodynamics up to approximate next-to-next-to-leading-order precision. No significant deviations are observed relative to the standard model predictions.

50 data tables

Normalized differential tt cross section (from l+jets channel) as a function of the transverse momentum pt of the lepton. The results are presented at particle level in the fiducial phase space. The statistical and systematic uncertainties are added in quadrature to yield the total uncertainty.

Normalized differential tt cross section (from l+jets channel) as a function of the pseudo-rapidity of the lepton. The results are presented at particle level in the fiducial phase space. The statistical and systematic uncertainties are added in quadrature to yield the total uncertainty.

Normalized differential tt cross section (from l+jets channel) as a function of the transverse momentum pt(b-jet) of the b-jet. The results are presented at particle level in the fiducial phase space. The statistical and systematic uncertainties are added in quadrature to yield the total uncertainty.

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Differential top-antitop cross-section measurements as a function of observables constructed from final-state particles using pp collisions at $\sqrt{s}=7$ TeV in the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 06 (2015) 100, 2015.
Inspire Record 1345452 DOI 10.17182/hepdata.77064

Various differential cross-sections are measured in top-quark pair ($t\bar{t}$) events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of $4.6$ fb$^{-1}$. The differential cross-sections are presented in terms of kinematic variables, such as momentum, rapidity and invariant mass, of a top-quark proxyreferred to as the pseudo-top-quark as well as the pseudo-top-quark pair system. The dependence of the measurement on theoretical models is minimal. The measurements are performed on $t\bar{t}$ events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a $b$-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the $W$ boson produced by the top-quark decay in events with a single charged lepton. Differential cross-section measurements of the pseudo-top-quark variables are compared with several Monte Carlo models that implement next-to-leading order or leading-order multi-leg matrix-element calculations.

21 data tables

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$in the muon channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.

Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $|y(\hat{t}_{\mathrm{h}})|$ in the muon channel. The results shown in this table are one of the inputs for the combined results.

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Measurement of the $t\bar{t}$ production cross-section as a function of jet multiplicity and jet transverse momentum in 7 TeV proton-proton collisions with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 01 (2015) 020, 2015.
Inspire Record 1304688 DOI 10.17182/hepdata.18665

The $t\bar{t}$ production cross-section dependence on jet multiplicity and jet transverse momentum is reported for proton--proton collisions at a centre-of-mass energy of 7 TeV in the single-lepton channel. The data were collected with the ATLAS detector at the CERN Large Hadron Collider and comprise the full 2011 data sample corresponding to an integrated luminosity of 4.6 fb$^{-1}$. Differential cross-sections are presented as a function of the jet multiplicity for up to eight jets using jet transverse momentum thresholds of 25, 40, 60, and 80 GeV, and as a function of jet transverse momentum up to the fifth jet. The results are shown after background subtraction and corrections for all detector effects, within a kinematic range closely matched to the experimental acceptance. Several QCD-based Monte Carlo models are compared with the results. Sensitivity to the parton shower modelling is found at the higher jet multiplicities, at high transverse momentum of the leading jet and in the transverse momentum spectrum of the fifth leading jet. The MC@NLO+HERWIG MC is found to predict too few events at higher jet multiplicities.

9 data tables

Measurement of the $t\overline{t}$ cross-section as a function of the jet multiplicity for jets with $p_{\mathrm{T}}$ larger than 25 GeV. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the jet multiplicity for jets with $p_{\mathrm{T}}$ larger than 40 GeV. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

Measurement of the $t\overline{t}$ cross-section as a function of the jet multiplicity for jets with $p_{\mathrm{T}}$ larger than 60 GeV. The uncertainties given correspond to the individual contributions of each source of systematic uncertainty as described in the paper.

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