A precise measurement of the Z-boson double-differential transverse momentum and rapidity distributions in the full phase space of the decay leptons with the ATLAS experiment at $\sqrt s$ = 8 TeV

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abeling, Kira ; et al.
Eur.Phys.J.C 84 (2024) 315, 2024.
Inspire Record 2698794 DOI 10.17182/hepdata.144246

This paper presents for the first time a precise measurement of the production properties of the Z boson in the full phase space of the decay leptons. The measurement is obtained from proton-proton collision data collected by the ATLAS experiment in 2012 at $\sqrt s$ = 8 TeV at the LHC and corresponding to an integrated luminosity of 20.2 fb$^{-1}$. The results, based on a total of 15.3 million Z-boson decays to electron and muon pairs, extend and improve a previous measurement of the full set of angular coefficients describing Z-boson decay. The double-differential cross-section distributions in Z-boson transverse momentum p$_T$ and rapidity y are measured in the pole region, defined as 80 $<$ m $<$ 100 GeV, over the range $|y| <$ 3.6. The total uncertainty of the normalised cross-section measurements in the peak region of the p$_T$ distribution is dominated by statistical uncertainties over the full range and increases as a function of rapidity from 0.5-1.0% for $|y| <$ 2.0 to 2-7% at higher rapidities. The results for the rapidity-dependent transverse momentum distributions are compared to state-of-the-art QCD predictions, which combine in the best cases approximate N$^4$LL resummation with N$^3$LO fixed-order perturbative calculations. The differential rapidity distributions integrated over p$_T$ are even more precise, with accuracies from 0.2-0.3% for $|y| <$ 2.0 to 0.4-0.9% at higher rapidities, and are compared to fixed-order QCD predictions using the most recent parton distribution functions. The agreement between data and predictions is quite good in most cases.

10 data tables

Measured $p_T$ cross sections in full-lepton phase space for |y| < 0.4.

Measured $p_T$ cross sections in full-lepton phase space for 0.4 < |y| < 0.8.

Measured $p_T$ cross sections in full-lepton phase space for 0.8 < |y| < 1.2.

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Inclusive-photon production and its dependence on photon isolation in $pp$ collisions at $\sqrt s=13$ TeV using 139 fb$^{-1}$ of ATLAS data

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abeling, Kira ; et al.
JHEP 07 (2023) 086, 2023.
Inspire Record 2628741 DOI 10.17182/hepdata.134100

Measurements of differential cross sections are presented for inclusive isolated-photon production in $pp$ collisions at a centre-of-mass energy of 13 TeV provided by the LHC and using 139 fb$^{-1}$ of data recorded by the ATLAS experiment. The cross sections are measured as functions of the photon transverse energy in different regions of photon pseudorapidity. The photons are required to be isolated by means of a fixed-cone method with two different cone radii. The dependence of the inclusive-photon production on the photon isolation is investigated by measuring the fiducial cross sections as functions of the isolation-cone radius and the ratios of the differential cross sections with different radii in different regions of photon pseudorapidity. The results presented in this paper constitute an improvement with respect to those published by ATLAS earlier: the measurements are provided for different isolation radii and with a more granular segmentation in photon pseudorapidity that can be exploited in improving the determination of the proton parton distribution functions. These improvements provide a more in-depth test of the theoretical predictions. Next-to-leading-order QCD predictions from JETPHOX and SHERPA and next-to-next-to-leading-order QCD predictions from NNLOJET are compared to the measurements, using several parameterisations of the proton parton distribution functions. The measured cross sections are well described by the fixed-order QCD predictions within the experimental and theoretical uncertainties in most of the investigated phase-space region.

48 data tables

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$ and photon isolation cone radius $R=0.4$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<0.8$ and photon isolation cone radius $R=0.4$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.8<|\eta^{\gamma}|<1.37$ and photon isolation cone radius $R=0.4$.

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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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Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abbott, Dale ; et al.
JHEP 11 (2021) 169, 2021.
Inspire Record 1887997 DOI 10.17182/hepdata.104925

A measurement of prompt photon-pair production in proton-proton collisions at $\sqrt{s}=13$ TeV is presented. The data were recorded by the ATLAS detector at the LHC with an integrated luminosity of 139 fb$^{-1}$. Events with two photons in the well-instrumented region of the detector are selected. The photons are required to be isolated and have a transverse momentum of $p_\mathrm{T,\gamma_{1(2)}} > 40(30)$ GeV for the leading (sub-leading) photon. The differential cross sections as functions of several observables for the diphoton system are measured and compared with theoretical predictions from state-of-the-art Monte Carlo and fixed-order calculations. The QCD predictions from next-to-next-to-leading-order calculations and multi-leg merged calculations are able to describe the measured integrated and differential cross sections within uncertainties, whereas lower-order calculations show significant deviations, demonstrating that higher-order perturbative QCD corrections are crucial for this process. The resummed predictions with parton showers additionally provide an excellent description of the low transverse-momentum regime of the diphoton system.

9 data tables

Differential cross section as a function of $p_{T,\gamma_{1}}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.

Differential cross section as a function of $p_{T,\gamma_{2}}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.

Integrated fiducial cross section measured in data and from different predictions.

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Version 2
Measurements of the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a $Z$ boson at $\sqrt{s} = 13$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Braden Keim ; Abbott, Dale ; et al.
Eur.Phys.J.C 81 (2021) 737, 2021.
Inspire Record 1853014 DOI 10.17182/hepdata.100351

Measurements of both the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a $Z$ boson ($t\bar{t}Z$) are presented. The measurements are performed by targeting final states with three or four isolated leptons (electrons or muons) and are based on $\sqrt{s} = 13$ TeV proton-proton collision data with an integrated luminosity of 139 fb$^{-1}$, recorded from 2015 to 2018 with the ATLAS detector at the CERN Large Hadron Collider. The inclusive cross section is measured to be $\sigma_{t\bar{t}Z} = 0.99 \pm 0.05$ (stat.) $\pm 0.08$ (syst.) pb, in agreement with the most precise theoretical predictions. The differential measurements are presented as a function of a number of kinematic variables which probe the kinematics of the $t\bar{t}Z$ system. Both absolute and normalised differential cross-section measurements are performed at particle and parton levels for specific fiducial volumes and are compared with theoretical predictions at different levels of precision, based on a $\chi^{2}/$ndf and $p$-value computation. Overall, good agreement is observed between the unfolded data and the predictions.

152 data tables

The measured $t\bar{t}\text{Z}$ cross-section value and its uncertainty based on the fit results from the combined trilepton and tetralepton channels. The value corresponds to the phase-space region where the difermion mass from the Z boson decay lies in the range $70 < m_{f\bar{f}} < 110$ GeV.

The measured $t\bar{t}\text{Z}$ cross-section value and its uncertainty based on the fit results from the combined trilepton and tetralepton channels. The value corresponds to the phase-space region where the difermion mass from the Z boson decay lies in the range $70 < m_{f\bar{f}} < 110$ GeV.

List of relative uncertainties of the measured inclusive $t\bar{t}\text{Z}$ cross section from the combined fit. The uncertainties are symmetrised for presentation and grouped into the categories described in the text. The quadratic sum of the individual uncertainties is not equal to the total uncertainty due to correlations introduced by the fit.

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Version 2
Measurement of hadronic event shapes in multijet final states at $\sqrt{s}=13$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
JHEP 01 (2021) 188, 2021.
Inspire Record 1808726 DOI 10.17182/hepdata.91998

A measurement of event-shape variables in proton$-$proton collisions at large momentum transfer is presented using data collected at $\sqrt{s} = 13$ TeV with the ATLAS detector at the Large Hadron Collider. Six event-shape variables calculated using hadronic jets are studied in inclusive multijet events using data corresponding to an integrated luminosity of 139 fb$^{-1}$. Measurements are performed in bins of jet multiplicity and in different ranges of the scalar sum of the transverse momenta of the two leading jets, reaching scales beyond 2 TeV. These measurements are compared with predictions from Monte Carlo event generators containing leading-order or next-to-leading order matrix elements matched to parton showers simulated to leading-logarithm accuracy. At low jet multiplicities, shape discrepancies between the measurements and the Monte Carlo predictions are observed. At high jet multiplicities, the shapes are better described but discrepancies in the normalisation are observed.

294 data tables

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.

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Measurements of inclusive and differential cross-sections of combined $t\bar{t}\gamma$ and $tW\gamma$ production in the $e\mkern-2mu\mu$ channel at 13 TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
JHEP 09 (2020) 049, 2020.
Inspire Record 1806806 DOI 10.17182/hepdata.94915

Inclusive and differential cross-sections for the production of top quarks in association with a photon are measured with proton$-$proton collision data corresponding to an integrated luminosity of 139 fb$^{-1}$. The data were collected by the ATLAS detector at the LHC during Run 2 between 2015 and 2018 at a centre-of-mass energy of 13 TeV. The measurements are performed in a fiducial volume defined at parton level. Events with exactly one photon, one electron and one muon of opposite sign, and at least two jets, of which at least one is $b$-tagged, are selected. The fiducial cross-section is measured to be $39.6\,^{+2.7}_{-2.3}\,\textrm{fb}$. Differential cross-sections as functions of several observables are compared with state-of-the-art Monte Carlo simulations and next-to-leading-order theoretical calculations. These include cross-sections as functions of photon kinematic variables, angular variables related to the photon and the leptons, and angular separations between the two leptons in the event. All measurements are in agreement with the predictions from the Standard Model.

24 data tables

The measured fiducial cross-section in the electron-muon channel. The first uncertainty is the statistical uncertainty and the second one is the systematic uncertainty.

The absolute differential cross-section measured in the fiducial phase-space as a function of the photon pT in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

The absolute differential cross-section measured in the fiducial phase-space as a function of the photon $|\eta|$ in the electron-muon channel. The uncertainty is decomposed into four components which are the signal modelling uncertainty, the background modelling uncertainty, the experimental uncertainty, and the data statistical uncertainty.

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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 isolated-photon plus two-jet production in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
JHEP 03 (2020) 179, 2020.
Inspire Record 1772071 DOI 10.17182/hepdata.101751

The dynamics of isolated-photon plus two-jet production in $pp$ collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, $\gamma+jet+jet$. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as the next-to-leading-order QCD predictions from SHERPA are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.

27 data tables

Measured cross sections for isolated-photon plus two-jet production as functions of $E_{\mathrm{T}}^{\gamma}$ for the total phase-space. The predictions from Sherpa NLO are also included.

Measured cross sections for isolated-photon plus two-jet production as functions of $p_{\mathrm{T}}^{\textrm{jet}}$ for the total phase-space. The predictions from Sherpa NLO are also included.

Measured cross sections for isolated-photon plus two-jet production as functions of $|y^{\textrm{jet}}|$ for the total phase-space. The predictions from Sherpa NLO are also included.

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Version 3
Measurement of the transverse momentum distribution of Drell-Yan lepton pairs in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
Eur.Phys.J.C 80 (2020) 616, 2020.
Inspire Record 1768911 DOI 10.17182/hepdata.92377

This paper describes precision measurements of the transverse momentum $p_\mathrm{T}^{\ell\ell}$ ($\ell=e,\mu$) and of the angular variable $\phi^{*}_{\eta}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton-proton collisions at $\sqrt{s}=$7 and 8 TeV, these new measurements probe perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. They reach a precision of 0.2% for the normalized spectra at low values of $p_\mathrm{T}^{\ell\ell}$. The data are compared with different QCD predictions, where it is found that predictions based on resummation approaches can describe the full spectrum within uncertainties.

80 data tables

Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.

Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.

Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.

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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 the inclusive isolated-photon cross section in $pp$ collisions at $\sqrt{s}=13$ TeV using 36 fb$^{-1}$ of ATLAS data

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abbott, Dale Charles ; et al.
JHEP 10 (2019) 203, 2019.
Inspire Record 1748270 DOI 10.17182/hepdata.91968

The differential cross section for isolated-photon production in $pp$ collisions is measured at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC using an integrated luminosity of 36.1 fb$^{-1}$. The differential cross section is presented as a function of the photon transverse energy in different regions of photon pseudorapidity. The differential cross section as a function of the absolute value of the photon pseudorapidity is also presented in different regions of photon transverse energy. Next-to-leading-order QCD calculations from JETPHOX and SHERPA as well as next-to-next-to-leading-order QCD calculations from NNLOJET are compared with the measurement, using several parameterisations of the proton parton distribution functions. The predictions provide a good description of the data within the experimental and theoretical uncertainties.

8 data tables

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

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Measurement of fiducial and differential $W^+W^-$ production cross-sections at $\sqrt{s}=$13 TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 79 (2019) 884, 2019.
Inspire Record 1734263 DOI 10.17182/hepdata.89225

A measurement of fiducial and differential cross-sections for $W^+W^-$ production in proton-proton collisions at $\sqrt{s}=$13 TeV with the ATLAS experiment at the Large Hadron Collider using data corresponding to an integrated luminosity of $36.1$ fb$^{-1}$ is presented. Events with one electron and one muon are selected, corresponding to the decay of the diboson system as $WW\rightarrow e^{\pm}\nu\mu^{\mp}\nu$. To suppress top-quark background, events containing jets with a transverse momentum exceeding 35 GeV are not included in the measurement phase space. The fiducial cross-section, six differential distributions and the cross-section as a function of the jet-veto transverse momentum threshold are measured and compared with several theoretical predictions. Constraints on anomalous electroweak gauge boson self-interactions are also presented in the framework of a dimension-six effective field theory.

43 data tables

Measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.

Statistical correlation between bins in data for the measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.

Total correlation between bins in data for the measured fiducial cross-section as a function of the jet-veto $p_{T}$ threshold. The value at the jet-veto $p_{T}$ threshold of 35GeV corresponds to the nominal fiducial cross section measured in this publication.

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Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 796 (2019) 230-252, 2019.
Inspire Record 1723858 DOI 10.17182/hepdata.87256

The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_\mathrm{NN}} = 8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{-1}$ recorded in 2016. The cross-section and nuclear modification factor $R_{p\mathrm{Pb}}$ are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (-2.83,-2.02), (-1.84,0.91), and (1.09,1.90). The cross-section and $R_{p\mathrm{Pb}}$ values are compared with the results of a next-to-leading-order perturbative QCD calculation, with and without nuclear parton distribution function modifications, and with expectations based on a model of the energy loss of partons prior to the hard scattering. The data disfavour a large amount of energy loss and provide new constraints on the parton densities in nuclei.

7 data tables

The measured cross sections for prompt, isolated photons with rapidity in (1.09,1.90).

The measured cross sections for prompt, isolated photons with rapidity in (−1.84,0.91).

The measured cross sections for prompt, isolated photons with rapidity in (−2.83,−2.02).

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Measurement of the ratio of cross sections for inclusive isolated-photon production in $pp$ collisions at $\sqrt s = 13$ and $8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 04 (2019) 093, 2019.
Inspire Record 1717495 DOI 10.17182/hepdata.89370

The ratio of the cross sections for inclusive isolated-photon production in $pp$ collisions at centre-of-mass energies of 13 and 8 TeV is measured using the ATLAS detector at the LHC. The integrated luminosities of the 13 TeV and 8 TeV datasets are 3.2 fb$^{-1}$ and 20.2 fb$^{-1}$, respectively. The ratio is measured as a function of the photon transverse energy in different regions of the photon pseudorapidity. The predictions from next-to-leading-order perturbative QCD calculations are compared with the measured ratio. The experimental systematic uncertainties as well as the uncertainties affecting the predictions are evaluated taking into account the correlations between the two centre-of-mass energies, resulting in a reduction of up to a factor of $2.5$ ($5$) in the experimental (theoretical) systematic uncertainties. The predictions based on several parameterisations of the proton parton distribution functions agree with the data within the reduced experimental and theoretical uncertainties. In addition, this ratio to that of the fiducial cross sections for $Z$ boson production at 13 and 8 TeV using the decay channels $Z \rightarrow e^+e^-$ and $Z \rightarrow \mu^+\mu^-$ is made and compared with the theoretical predictions. In this double ratio, a further reduction of the experimental uncertainty is obtained because the uncertainties arising from the luminosity measurement cancel out. The predictions describe the measurements of the double ratio within the theoretical and experimental uncertainties.

16 data tables

Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Predicted ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Measured ratio of cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

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Measurements of inclusive and differential fiducial cross-sections of $t\bar{t}\gamma$ production in leptonic final states at $\sqrt{s}$ = 13 TeV in ATLAS

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 79 (2019) 382, 2019.
Inspire Record 1707015 DOI 10.17182/hepdata.88061

Inclusive and differential cross-sections for the production of a top-quark pair in association with a photon are measured with proton-proton collision data corresponding to an integrated luminosity of 36.1 fb$^{-1}$, collected by the ATLAS detector at the LHC in 2015 and 2016 at a centre-of-mass energy of 13 TeV. The measurements are performed in single-lepton and dilepton final states in a fiducial volume. Events with exactly one photon, one or two leptons, a channel-dependent minimum number of jets, and at least one $b$-jet are selected. Neural network algorithms are used to separate the signal from the backgrounds. The fiducial cross-sections are measured to be 521 $\pm$ 9(stat.) $\pm$ 41(sys.) fb and 69 $\pm$ 3(stat.) $\pm$ 4(sys.) fb for the single-lepton and dilepton channels, respectively. The differential cross-sections are measured as a function of photon transverse momentum, photon absolute pseudorapidity, and angular distance between the photon and its closest lepton in both channels, as well as azimuthal opening angle and absolute pseudorapidity difference between the two leptons in the dilepton channel. All measurements are in agreement with the theoretical predictions.

20 data tables

The measured fiducial cross section in the single lepton channel. The first uncertainty is the statistical uncertainty and the second one is the systematic uncertainty.

The measured fiducial cross section in the dilepton channel. The first uncertainty is the statistical uncertainty and the second one is the systematic uncertainty.

The measured normalized differential cross section as a function of the photon pT in the single lepton channel. The uncertainty is decomposed into five components which are the signal modelling uncertainty, the experimental uncertainty, the ttbar modelling uncertainty, the other background estimation uncertainty, and the data statistical uncertainty.

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Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 780 (2018) 578-602, 2018.
Inspire Record 1645627 DOI 10.17182/hepdata.78401

The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 fb$^{-1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.

5 data tables

Measured cross sections for isolated-photon plus jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus jet production as a function of $p_{\rm T}^{\rm jet-lead}$.

Measured cross sections for isolated-photon plus jet production as a function of $\Delta\phi^{\rm \gamma-jet\ lead}$.

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Version 2
Measurement of the production cross section of three isolated photons in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 781 (2018) 55-76, 2018.
Inspire Record 1644367 DOI 10.17182/hepdata.80511

A measurement of the production of three isolated photons in proton-proton collisions at a centre-of-mass energy $\sqrt{s}$ = 8 TeV is reported. The results are based on an integrated luminosity of 20.2 fb$^{-1}$ collected with the ATLAS detector at the LHC. The differential cross sections are measured as functions of the transverse energy of each photon, the difference in azimuthal angle and in pseudorapidity between pairs of photons, the invariant mass of pairs of photons, and the invariant mass of the triphoton system. A measurement of the inclusive fiducial cross section is also reported. Next-to-leading-order perturbative QCD predictions are compared to the cross-section measurements. The predictions underestimate the measurement of the inclusive fiducial cross section and the differential measurements at low photon transverse energies and invariant masses. They provide adequate descriptions of the measurements at high values of the photon transverse energies, invariant mass of pairs of photons, and invariant mass of the triphoton system.

13 data tables

The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon1).

The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon2).

The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon3).

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Version 2
Measurement of differential cross-sections of a single top quark produced in association with a $W$ boson at $\sqrt{s}=13$ TeV with ATLAS

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 78 (2018) 186, 2018.
Inspire Record 1641076 DOI 10.17182/hepdata.81944

The differential cross-section for the production of a $W$ boson in association with a top quark is measured for several particle-level observables. The measurements are performed using 36.1 fb$^{-1}$ of $pp$ collision data collected with the ATLAS detector at the LHC in 2015 and 2016. Differential cross-sections are measured in a fiducial phase space defined by the presence of two charged leptons and exactly one jet matched to a $b$-hadron, and are normalised with the fiducial cross-section. Results are found to be in good agreement with predictions from several Monte Carlo event generators.

13 data tables

Fiducial region definition.

Absolute cross-sections differential in E(b). Uncertainties are signed to show correlations.

Absolute cross-sections differential in m(l1b). Uncertainties are signed to show correlations.

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Version 2
Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 05 (2018) 077, 2018.
Inspire Record 1635273 DOI 10.17182/hepdata.80076

This paper presents a measurement of the $W$ boson production cross section and the $W^{+}/W^{-}$ cross-section ratio, both in association with jets, in proton--proton collisions at $\sqrt{s}=8$ TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb$^{-1}$. Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the $W$ boson. For a subset of the observables, the differential cross sections of positively and negatively charged $W$ bosons are measured separately. In the cross-section ratio of $W^{+}/W^{-}$ the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proton.

86 data tables

Cross section for the production of W bosons for different inclusive jet multiplicities.

Statistical correlation between bins in data for the cross section for the production of W bosons for different inclusive jet multiplicities.

Differential cross sections for the production of W<sup>+</sup> bosons, W<sup>-</sup> bosons and the W<sup>+</sup>/W<sup>-</sup> cross section ratio as a function of the inclusive jet multiplicity.

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Version 3
Measurement of the Drell--Yan triple-differential cross section in $pp$ collisions at $\sqrt{s} = 8$ TeV

The ATLAS collaboration Aaboud, M. ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 12 (2017) 059, 2017.
Inspire Record 1630886 DOI 10.17182/hepdata.77492

This paper presents a measurement of the triple-differential cross section for the Drell--Yan process $Z/\gamma^*\rightarrow \ell^+\ell^-$ where $\ell$ is an electron or a muon. The measurement is performed for invariant masses of the lepton pairs, $m_{\ell\ell}$, between $46$ and $200$ GeV using a sample of $20.2$ fb$^{-1}$ of $pp$ collisions data at a centre-of-mass energy of $\sqrt{s}=8$ TeV collected by the ATLAS detector at the LHC in 2012. The data are presented in bins of invariant mass, absolute dilepton rapidity, $|y_{\ell\ell}|$, and the angular variable $\cos\theta^{*}$ between the outgoing lepton and the incoming quark in the Collins--Soper frame. The measurements are performed in the range $|y_{\ell\ell}|<2.4$ in the muon channel, and extended to $|y_{\ell\ell}|<3.6$ in the electron channel. The cross sections are used to determine the $Z$ boson forward-backward asymmetry as a function of $|y_{\ell\ell}|$ and $m_{\ell\ell}$. The measurements achieve high-precision, below the percent level in the pole region, excluding the uncertainty in the integrated luminosity, and are in agreement with predictions. These precision data are sensitive to the parton distribution functions and the effective weak mixing angle.

20 data tables

Detailed breakdown of systematic uncertainties for the measurement in the central rapidity muon channel. Common systematic uncertainty on the luminosity measurment of 1.8% is not included. Correlated systematic uncertainties with the suffix :A should be treated as additive and with the suffix :M should be treated as multiplicative. The source 'sys,uncor' represents bin-to-bin uncorrelated systematic uncertainty. The cross sections are given at the Born QED level. 'C Dressed' represents the multiplicative correction factor to translate the cross sections to the dressed level with the cone radius of 0.1: SigmaDressed = C Dressed * SigmaBorn.

Detailed breakdown of systematic uncertainties for the measurement in the central rapidity muon channel. Common systematic uncertainty on the luminosity measurment of 1.8% is not included. Correlated systematic uncertainties with the suffix :A should be treated as additive and with the suffix :M should be treated as multiplicative. The source 'sys,uncor' represents bin-to-bin uncorrelated systematic uncertainty. The cross sections are given at the Born QED level. 'C Dressed' represents the multiplicative correction factor to translate the cross sections to the dressed level with the cone radius of 0.1: SigmaDressed = C Dressed * SigmaBorn.

Detailed breakdown of systematic uncertainties for the measurement in the central rapidity muon channel. Common systematic uncertainty on the luminosity measurment of 1.8% is not included. Correlated systematic uncertainties with the suffix :A should be treated as additive and with the suffix :M should be treated as multiplicative. The source 'sys,uncor' represents bin-to-bin uncorrelated systematic uncertainty. The cross sections are given at the Born QED level. 'C Dressed' represents the multiplicative correction factor to translate the cross sections to the dressed level with the cone radius of 0.1: SigmaDressed = C Dressed * SigmaBorn.

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Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 10 (2017) 132, 2017.
Inspire Record 1615206 DOI 10.17182/hepdata.79497

Inclusive and differential fiducial cross sections of Higgs boson production in proton-proton collisions are measured in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel. The proton-proton collision data were produced at the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector in 2015 and 2016, corresponding to an integrated luminosity of 36.1 fb$^{-1}$. The inclusive fiducial cross section in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel is measured to be 3.62 $\pm$ 0.50 (stat) $^{+0.25}_{-0.20}$ (sys) fb, in agreement with the Standard Model prediction of 2.91 $\pm$ 0.13 fb. The cross section is also extrapolated to the total phase space including all Standard Model Higgs boson decays. Several differential fiducial cross sections are measured for observables sensitive to the Higgs boson production and decay, including kinematic distributions of jets produced in association with the Higgs boson. Good agreement is found between data and Standard Model predictions. The results are used to put constraints on anomalous Higgs boson interactions with Standard Model particles, using the pseudo-observable extension to the kappa-framework.

16 data tables

Measured differential fiducial cross sections in Higgs transverse momentum (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.

Measured differential fiducial cross sections in Higgs rapidity (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.

Measured differential fiducial cross sections in invariant mass of the subleading lepton pair (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.

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Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Rev.D 95 (2017) 112005, 2017.
Inspire Record 1591327 DOI 10.17182/hepdata.77381

A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of $\sqrt{s}=8$ TeV is presented. The results are based on an integrated luminosity of 20.2 fb$^{-1}$ recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying $|\eta^{\gamma}|<1.37$ or ${1.56<|\eta^{\gamma}|<2.37}$ and transverse energies of respectively $E_{\mathrm{T,1}}^{\gamma}>40$ GeV and $E_{\mathrm{T,2}}^{\gamma}>30$ GeV for the two leading photons ordered in transverse energy produced in the interaction.The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is $16.8 \pm 0.8$ pb. The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%.

7 data tables

The measured fiducial (total xs).

The measured differential as a function of Mgg.

The measured differential as a function of pTgg.

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Measurement of the cross section for inclusive isolated-photon production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 770 (2017) 473-493, 2017.
Inspire Record 1510441 DOI 10.17182/hepdata.79798

Inclusive isolated-photon production in $pp$ collisions at a centre-of-mass energy of 13 TeV is studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2 fb$^{-1}$. The cross section is measured as a function of the photon transverse energy above 125 GeV in different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data.

8 data tables

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.

Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.

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High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Nucl.Phys.B 918 (2017) 257-316, 2017.
Inspire Record 1499475 DOI 10.17182/hepdata.79948

The dynamics of isolated-photon plus one-, two- and three-jet production in $pp$ collisions at a centre-of-mass energy of 8 TeV are studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 20.2 fb$^{-1}$. Measurements of isolated-photon plus jets cross sections are presented as functions of the photon and jet transverse momenta. The cross sections as functions of the azimuthal angle between the photon and the jets, the azimuthal angle between the jets, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system are presented. The pattern of QCD radiation around the photon and the leading jet is investigated by measuring jet production in an annular region centred on each object; enhancements are observed around the leading jet with respect to the photon in the directions towards the beams. The experimental measurements are compared to several different theoretical calculations, and overall a good description of the data is found.

35 data tables

Measured cross sections for isolated-photon plus 1jet production as a function of $E_{\rm T}^{\gamma}$.

Measured cross sections for isolated-photon plus 1jet production as a function of $p_{\rm T}^{\rm jet1}$.

Measured cross sections for isolated-photon plus 1jet production as a function of $m^{\gamma-\rm jet1}$.

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Measurement of $W$ boson angular distributions in events with high transverse momentum jets at $\sqrt{s}=$ 8 TeV using the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 765 (2017) 132-153, 2017.
Inspire Record 1487726 DOI 10.17182/hepdata.74701

The $W$ boson angular distribution in events with high transverse momentum jets is measured using data collected by the ATLAS experiment from proton-proton collisions at a centre-of-mass energy $\sqrt{s}=$ 8 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 20.3 fb$^{-1}$. The focus is on the contributions to $W$ + jets processes from real $W$ emission, which is achieved by studying events where a muon is observed close to a high transverse momentum jet. At small angular separations, these contributions are expected to be large. Various theoretical models of this process are compared to the data in terms of the absolute cross-section and the angular distributions of the muon from the leptonic $W$ decay.

5 data tables

Measured integrated cross-sections as a function of leading jet transverse momentum for the collinear region ($0.2 < \Delta R < 2.4$), the back-to-back region ($\Delta R > 2.4$) and inclusively.

Measured cross-section as a function of angular separation between the muon and the closest jet. Multiplicative correction factors for using prompt muons and prompt dressing photons in the particle-level selection, derived from ALPGEN 2.14 interfaced with PYTHIA 6.426, are also shown.

Breakdown of uncertainties in percent.

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Study of hard double-parton scattering in four-jet events in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS experiment

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
JHEP 11 (2016) 110, 2016.
Inspire Record 1479760 DOI 10.17182/hepdata.73908

Inclusive four-jet events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV are analysed for the presence of hard double-parton scattering using data corresponding to an integrated luminosity of 37.3 pb$^{-1}$, collected with the ATLAS detector at the LHC. The contribution of hard double-parton scattering to the production of four-jet events is extracted using an artificial neural network, assuming that hard double-parton scattering can be approximated by an uncorrelated overlaying of dijet events. For events containing at least four jets with transverse momentum $p_{\mathrm{T}} \geq 20$ GeV and pseudorapidity $\eta \leq 4.4$, and at least one having $p_{\mathrm{T}} \geq 42.5$ GeV, the contribution of hard double-parton scattering is estimated to be $f_{\mathrm{DPS}} = 0.092 ^{+0.005}_{-0.011} (\mathrm{stat.}) ^{+0.033}_{-0.037} (\mathrm{syst.})$. After combining this measurement with those of the inclusive dijet and four-jet cross-sections in the appropriate phase space regions, the effective overlap area between the interacting protons, $\sigma_{\mathrm{eff}}$, was determined to be $\sigma_{\mathrm{eff}} = 14.9 ^{+1.2}_{-1.0} (\mathrm{stat.}) ^{+5.1}_{-3.8} (\mathrm{syst.})$ mb. This result is consistent within the quoted uncertainties with previous measurements of $\sigma_{\mathrm{eff}}$, performed at centre-of-mass energies between 63 GeV and 8 TeV using various final states, and it corresponds to $21^{+7}_{-6}$% of the total inelastic cross-section measured at $\sqrt{s} = 7$ TeV. The distributions of the observables sensitive to the contribution of hard double-parton scattering, corrected for detector effects, are also provided.

21 data tables

Normalized distribution of the variable $\Delta^{p_{\mathrm{T}}}_{34}$, defined in Eq (16) of the paper, in data after unfolding to particle level.

Normalized distribution of the variable $\Delta\phi_{34}$, defined in Eq (16) of the paper, in data after unfolding to particle level.

Normalized distribution of the variable $\Delta^{p_{\mathrm{T}}}_{12}$, defined in Eq (16) of the paper, in data after unfolding to particle level.

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Measurement of the $b\overline{b}$ dijet cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Eur.Phys.J.C 76 (2016) 670, 2016.
Inspire Record 1478355 DOI 10.17182/hepdata.75316

The dijet production cross section for jets containing a $b$-hadron ($b$-jets) has been measured in proton-proton collisions with a centre-of-mass energy of $\sqrt{s} = 7$ TeV, using the ATLAS detector at the LHC. The data used correspond to an integrated luminosity of 4.2 fb$^{-1}$. The cross section is measured for events with two identified $b$-jets with a transverse momentum $p_T > 20$ GeV and a minimum separation in the $\eta$-$\phi$ plane of $\Delta R = 0.4$. At least one of the jets in the event is required to have $p_T > 270$ GeV. The cross section is measured differentially as a function of dijet invariant mass, dijet transverse momentum, boost of the dijet system, and the rapidity difference, azimuthal angle and angular distance between the $b$-jets. The results are compared to different predictions of leading order and next-to-leading order perturbative quantum chromodynamics matrix elements supplemented with models for parton-showers and hadronization.

6 data tables

Results for the m_bb distribution. Statistical and systematic uncertainties are quoted.

Results for the DeltaPhi distribution. Statistical and systematic uncertainties are quoted.

Results for the y* distribution. Statistical and systematic uncertainties are quoted.

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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 total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

The ATLAS collaboration Aaboud, Morad ; Aad, Georges ; Abbott, Brad ; et al.
Phys.Lett.B 761 (2016) 158-178, 2016.
Inspire Record 1477585 DOI 10.17182/hepdata.73997

A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=8$ TeV is presented. An integrated luminosity of $500$ $\mu$b$^{-1}$ was accumulated in a special run with high-$\beta^{\star}$ beam optics to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $-t$ range from $0.014$ GeV$^2$ to $0.1$ GeV$^2$ to extrapolate $t\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $\sigma_{\mathrm{tot}}(pp\rightarrow X) = {96.07} \; \pm 0.18 \; ({{stat.}}) \pm 0.85 \; ({{exp.}}) \pm 0.31 \; ({extr.}) \; {mb} \;,$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation $t\rightarrow 0$. In addition, the slope of the exponential function describing the elastic cross section at small $t$ is determined to be $B = 19.74 \pm 0.05 \; ({{stat.}}) \pm 0.23 \; ({{syst.}}) \; {GeV}^{-2}$.

6 data tables

The measured total cross section, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t-->0.

The nuclear slope of the differential eslastic cross section at small |t|, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t-->0.

The total elastic cross section and the observed elastic cross section within the fiducial volume.

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Measurement of the $W^{\pm}Z$ boson pair-production cross section 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 762 (2016) 1-22, 2016.
Inspire Record 1469071 DOI 10.17182/hepdata.76493

The production of $W^{\pm}Z$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb$^{-1}$. The $W^{\pm}Z$ candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is $\sigma_{W^\pm Z \rightarrow \ell^{'} \nu \ell \ell}^{\textrm{fid.}} = 63.2 \pm 3.2$ (stat.) $\pm 2.6$ (sys.) $\pm 1.5$ (lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is $53.4^{+3.6}_{-2.8}$ fb. The extrapolation of the measurement from the fiducial to the total phase space yields $\sigma_{W^{\pm}Z}^{\textrm{tot.}} = 50.6 \pm 2.6$ (stat.) $\pm 2.0$ (sys.) $\pm 0.9$ (th.) $\pm 1.2$ (lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of $48.2^{+1.1}_{-1.0}$ pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent $W^+Z$ and $W^-Z$ cross sections and their ratio.

11 data tables

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

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Measurement of the double-differential high-mass Drell-Yan cross section in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 08 (2016) 009, 2016.
Inspire Record 1467454 DOI 10.17182/hepdata.75023

This paper presents a measurement of the double-differential cross section for the Drell-Yan $Z/\gamma^{*} \rightarrow \ell^{+} \ell^{-}$ and photon-induced $\gamma\gamma \rightarrow \ell^{+} \ell^{-}$ processes where $\ell$ is an electron or muon. The measurement is performed for invariant masses of the lepton pairs, $m_{\ell\ell}$, between 116 GeV and 1500 GeV, using a sample of 20.3 fb$^{-1}$ of pp collisions data at centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the LHC in 2012. The data are presented double differentially in invariant mass and absolute dilepton rapidity as well as in invariant mass and absolute pseudorapidity separation of the lepton pair. The single-differential cross section as a function of $m_{\ell\ell}$ is also reported. The electron and muon channel measurements are combined and a total experimental precision of better than 1% is achieved at low $m_{\ell\ell}$. A comparison to next-to-next-to-leading order perturbative QCD predictions using several recent parton distribution functions and including next-to-leading order electroweak effects indicates the potential of the data to constrain parton distribution functions. In particular, a large impact of the data on the photon PDF is demonstrated.

39 data tables

The combined Born-level single-differential cross section as a function of invariant mass. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".

The combined Born-level double-differential cross section as a function of invariant mass and absolute rapidity. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".

The combined Born-level double-differential cross section as a function of invariant mass and absolute pseudorapidity separation of the leptons. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".

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Measurement of the inclusive isolated prompt photon cross section in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 08 (2016) 005, 2016.
Inspire Record 1457605 DOI 10.17182/hepdata.76985

A measurement of the cross section for the inclusive production of isolated prompt photons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV is presented. The measurement covers the pseudo rapidity ranges $|\eta^{\gamma}| < 1.37$ and $1.56 \leq |\eta^{\gamma}| < 2.37$ in the transverse energy range $25 < E_{\rm T}^{\gamma} < 1500$ GeV. The results are based on an integrated luminosity of 20.2 fb$^{-1}$, recorded by the ATLAS detector at the LHC. Photon candidates are identified by combining information from the calorimeters and the inner tracker. The background is subtracted using a data-driven technique, based on the observed calorimeter shower-shape variables and the deposition of hadronic energy in a narrow cone around the photon candidate. The measured cross sections are compared with leading-order and next-to-leading order perturbative QCD calculations and are found to be in a good agreement over ten orders of magnitude.

4 data tables

The inclusive prompt photon cross section with systematic and statistical uncertainties for the region |eta(gamma)| < 0.6.

The inclusive prompt photon cross section with systematic and statistical uncertainties for the region 0.6<|eta(gamma)| < 1.37.

The inclusive prompt photon cross section with systematic and statistical uncertainties for the region 1.56<|eta(gamma)| < 1.81.

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Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to $WW^{\ast}{\rightarrow\,}e\nu\mu\nu$ with the ATLAS detector at $\sqrt{s}=8$ TeV

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 08 (2016) 104, 2016.
Inspire Record 1444991 DOI 10.17182/hepdata.76843

This paper describes a measurement of fiducial and differential cross sections of gluon-fusion Higgs boson production in the $H{\rightarrow\,}WW^{\ast}{\rightarrow\,}e\nu\mu\nu$ channel, using 20.3 fb$^{-1}$ of proton-proton collision data. The data were produced at a centre-of-mass energy of $\sqrt{s} = 8$ TeV at the CERN Large Hadron Collider and recorded by the ATLAS detector in 2012. Cross sections are measured from the observed $H{\rightarrow\,}WW^{\ast}{\rightarrow\,}e\nu\mu\nu$ signal yield in categories distinguished by the number of associated jets. The total cross section is measured in a fiducial region defined by the kinematic properties of the charged leptons and neutrinos. Differential cross sections are reported as a function of the number of jets, the Higgs boson transverse momentum, the dilepton rapidity, and the transverse momentum of the leading jet. The jet-veto efficiency, or fraction of events with no jets above a given transverse momentum threshold, is also reported. All measurements are compared to QCD predictions from Monte Carlo generators and fixed-order calculations, and are in agreement with the Standard Model predictions.

22 data tables

Measured total fiducial cross section in fb.

Measured fiducial cross section in fb as a function of Njet. Jet PT>25 GeV for |eta|<2.4 and PT>30 GeV for 2.4<|eta|<4.5.

Measured fiducial cross section in fb/GeV as a function of pTH.

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Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Rev.D 93 (2016) 092004, 2016.
Inspire Record 1426523 DOI 10.17182/hepdata.75197

This paper presents measurements of $W^\pm Z$ production in $pp$ collisions at a center-of-mass energy of 8 TeV. The gauge bosons are reconstructed using their leptonic decay modes into electrons and muons. The data were collected in 2012 by the ATLAS experiment at the Large Hadron Collider, and correspond to an integrated luminosity of 20.3 fb$^{-1}$. The measured inclusive cross section in the detector fiducial region is $\sigma_{W^\pm Z \rightarrow \ell^{'} \nu\ \ell \ell} = 35.1 \pm$ 0.9 (stat.) $\pm 0.8$ (sys.) $\pm 0.8$ (lumi.) fb, for one leptonic decay channel. In comparison, the next-to-leading-order Standard Model expectation is 30.0 $\pm$ 2.1 fb. Cross sections for $W^+Z$ and $W^-Z$ production and their ratio are presented as well as differential cross sections for several kinematic observables. Limits on anomalous triple gauge boson couplings are derived from the transverse mass spectrum of the $W^\pm Z$ system. From the analysis of events with a $W$ and a $Z$ boson associated with two or more forward jets an upper limit at 95% confidence level on the $W^\pm Z$ scattering cross section of 0.63 fb, for each leptonic decay channel, is established, while the Standard Model prediction at next-to-leading order is 0.13 fb. Limits on anomalous quartic gauge boson couplings are also extracted.

48 data tables

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.

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Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
JHEP 09 (2016) 029, 2016.
Inspire Record 1426515 DOI 10.17182/hepdata.76808

The production of $W$ boson pairs in proton-proton collisions at $\sqrt{s}=$ 8 TeV is studied using data corresponding to 20.3 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The $W$ bosons are reconstructed using their leptonic decays into electrons or muons and neutrinos. Events with reconstructed jets are not included in the candidate event sample. A total of 6636 $WW$ candidate events are observed. Measurements are performed in fiducial regions closely approximating the detector acceptance. The integrated measurement is corrected for all acceptance effects and for the $W$ branching fractions to leptons in order to obtain the total $WW$ production cross section, which is found to be 71.1$\pm1.1$(stat)$^{+5.7}_{-5.0}$(syst)$\pm1.4$ pb. This agrees with the next-to-next-to-leading-order Standard Model prediction of 63.2$^{+1.6}_{-1.4}$(scale)$\pm1.2$(PDF) pb. Fiducial differential cross sections are measured as a function of each of six kinematic variables. The distribution of the transverse momentum of the leading lepton is used to set limits on anomalous triple-gauge-boson couplings.

29 data tables

Measured production cross sections of WW production in the fiducial region for different final states corresponding to different W decay channels: both W's decaying into electrons or both decaying to muon. The cross sections are defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)<2.47 and to lie outside of 1.37 < abs(eta) < 1.53, muons are required to lie within abs(eta)<2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 45 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos multiplied by the sine of azimuthal difference between lepton and the vectorial sum of the neutrinos in the event should be larger than 45 GeV if the azimuthal difference between lepton and the vectorial sum of the neutrinos is smaller than PI/2. The invariant mass of the leptons should exceed 15 GeV. The absolute difference between the invariant mass of the leptons and the mass of the Z boson should be larger than 15 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)<4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.

Measured production cross section of WW production in the fiducial region in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)<2.47 and to lie outside of 1.37 < abs(eta) < 1.53, muons are required to lie within abs(eta)<2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)<4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.

Measured total production cross sections of WW production in the total phase space. Both, resonant and non-resonant WW, production are considered as signal.

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Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Nucl.Phys.B 907 (2016) 717-763, 2016.
Inspire Record 1408878 DOI 10.17182/hepdata.77020

The production of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ charmed mesons has been measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV at the LHC, using data corresponding to an integrated luminosity of $280\,$nb$^{-1}$. The charmed mesons have been reconstructed in the range of transverse momentum $3.5<p_{\rm T}(D)<100$ GeV and pseudorapidity $|\eta(D)|<2.1$. The differential cross sections as a function of transverse momentum and pseudorapidity were measured for $D^{*\pm}$ and $D^\pm$ production. The next-to-leading-order QCD predictions are consistent with the data in the visible kinematic region within the large theoretical uncertainties. Using the visible $D$ cross sections and an extrapolation to the full kinematic phase space, the strangeness-suppression factor in charm fragmentation, the fraction of charged non-strange $D$ mesons produced in a vector state, and the total cross section of charm production at $\sqrt{s}=7$ TeV were derived.

4 data tables

The visible low-$p_T$, $3.5<p_T(D)<20\rm{\ GeV}$, and high-$p_T$, $20<p_T(D)<100\rm{\ GeV}$, cross sections of $D^{*\pm}$, $D^\pm$ and $D^\pm_s$ production with $|\eta|<2.1$. The data uncertainties are the total uncertainties obtained as sums in quadrature of the statistical, systematic, luminosity and branching-fraction uncertainties.

The measured differential cross sections $\rm{d}\sigma/\rm{d}p_T$ of $D^{*\pm}$ and $D^\pm$ production with $|\eta|<2.1$. The first and second errors are the statistical and systematic uncertainties, respectively. The systematic uncertainties corresponding to the tracking ($\delta_2$) uncertainties (Table 2 of the paper) are strongly correlated. The fully correlated uncertainties linked with the luminosity measurement ($3.5\%$) and branching fractions ($1.5\%$ and $2.1\%$ for $D^{*\pm}$ and $D^\pm$, respectively) are not shown.

The measured differential cross sections $\rm{d}\sigma/\rm{d}|\eta|$ of $D^{*\pm}$ and $D^\pm$ production with $3.5<p_T<20\,$GeV. The first and second errors are the statistical and systematic uncertainties, respectively. The systematic uncertainty fractions corresponding to the tracking ($\delta_2$) uncertainties (Table 2 of the paper) are strongly correlated. The fully correlated uncertainties linked with the luminosity measurement ($3.5\%$) and branching fractions ($1.5\%$ and $2.1\%$ for $D^{*\pm}$ and $D^\pm$, respectively) are not shown.

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


Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the $H \rightarrow \gamma \gamma$ and $H \rightarrow ZZ ^{*}\rightarrow 4\ell$ Decay Channels at $\sqrt{s}=8$ TeV with the ATLAS Detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Rev.Lett. 115 (2015) 091801, 2015.
Inspire Record 1364361 DOI 10.17182/hepdata.57334

Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3 fb$^{-1}$ of $pp$ collisions produced by the Large Hadron Collider at a center-of-mass energy of $\sqrt{s} = 8$ TeV and recorded by the ATLAS detector. Cross sections are obtained from measured $H \rightarrow \gamma \gamma$ and $H \rightarrow ZZ ^{*}\rightarrow 4\ell$ event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be $\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}$. The measurements are compared to state-of-the-art predictions.

17 data tables

Measured cross section in bins of $p_{\rm{T}}^{\rm{H}}$.

Measured cross section in bins of $|y^{\rm{H}}|$.

Measured cross section in bins of $N_{\rm{jets}}$.

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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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Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in $pp$ collisions at $\sqrt{s}$=8 TeV with the ATLAS detector

The ATLAS collaboration Aad, Georges ; Abbott, Brad ; Abdallah, Jalal ; et al.
Phys.Lett.B 738 (2014) 234-253, 2014.
Inspire Record 1310835 DOI 10.17182/hepdata.78567

Measurements of fiducial and differential cross sections of Higgs boson production in the ${H \rightarrow ZZ ^{*}\rightarrow 4\ell}$ decay channel are presented. The cross sections are determined within a fiducial phase space and corrected for detection efficiency and resolution effects. They are based on 20.3 fb$^{-1}$ of $pp$ collision data, produced at $\sqrt{s}$=8 TeV centre-of-mass energy at the LHC and recorded by the ATLAS detector. The differential measurements are performed in bins of transverse momentum and rapidity of the four-lepton system, the invariant mass of the subleading lepton pair and the decay angle of the leading lepton pair with respect to the beam line in the four-lepton rest frame, as well as the number of jets and the transverse momentum of the leading jet. The measured cross sections are compared to selected theoretical calculations of the Standard Model expectations. No significant deviation from any of the tested predictions is found.

6 data tables

Measured differential fiducial cross sections in Higgs transverse momentum (second column). The given uncertainty includes statistical and systematic components. The third (fourth) column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ (HRes) for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fifth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.

Measured differential fiducial cross sections in the absolute value of the Higgs rapidity (second column). The given uncertainty includes statistical and systematic components. The third (fourth) column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ (HRes) for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fifth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.

Measured differential fiducial cross sections in m34, which corresponds to the invariant mass of the off-shell Z boson (second column). The given uncertainty includes statistical and systematic components. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fourth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.

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