A search for nonresonant Higgs boson pair production in the $b\bar{b}\gamma\gamma$ final state is performed using 140 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. This analysis supersedes and expands upon the previous nonresonant ATLAS results in this final state based on the same data sample. The analysis strategy is optimised to probe anomalous values not only of the Higgs ($H$) boson self-coupling modifier $\kappa_\lambda$ but also of the quartic $HHVV$ ($V=W,Z$) coupling modifier $\kappa_{2V}$. No significant excess above the expected background from Standard Model processes is observed. An observed upper limit $\mu_{HH}<4.0$ is set at 95% confidence level on the Higgs boson pair production cross-section normalised to its Standard Model prediction. The 95% confidence intervals for the coupling modifiers are $-1.4<\kappa_\lambda<6.9$ and $-0.5<\kappa_{2V}<2.7$, assuming all other Higgs boson couplings except the one under study are fixed to the Standard Model predictions. The results are interpreted in the Standard Model effective field theory and Higgs effective field theory frameworks in terms of constraints on the couplings of anomalous Higgs boson (self-)interactions.
The acceptance times efficiency for the signal ggF $HH$ process in each analysis category as a function of the $c_{{H}\boxed{}}$ SMEFT coefficients. The dashed lines denote values that are excluded at 95% CL. The bottom panels show the efficiency of the sum of all analysis categories.
Statistical combinations of searches for charginos and neutralinos using various decay channels are performed using $139\,$fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=13\,$TeV with the ATLAS detector at the Large Hadron Collider. Searches targeting pure-wino chargino pair production, pure-wino chargino-neutralino production, or higgsino production decaying via Standard Model $W$, $Z$, or $h$ bosons are combined to extend the mass reach to the produced SUSY particles by 30-100 GeV. The depth of the sensitivity of the original searches is also improved by the combinations, lowering the 95% CL cross-section upper limits by 15%-40%.
Observed 95% CL exclusion limits on the simplified models of higgsino GGM scenarios.
A search for physics beyond the Standard Model inducing periodic signals in the dielectron and diphoton invariant mass spectra is presented using 139 fb$^{-1}$ of $\sqrt{s}=13$ TeV $pp$ collision data collected by the ATLAS experiment at the LHC. Novel search techniques based on continuous wavelet transforms are used to infer the frequency of periodic signals from the invariant mass spectra and neural network classifiers are used to enhance the sensitivity to periodic resonances. In the absence of a signal, exclusion limits are placed at the 95% confidence level in the two-dimensional parameter space of the clockwork gravity model. Model-independent searches for deviations from the background-only hypothesis are also performed.
The expected minus one standard deviation exclusion limit at 95% CL for the clockwork gravity model projected in the $k–M_{5}$ parameter space for the $\gamma\gamma$ channel for the case without mass thresholds.
This paper presents a study of $Z \to ll\gamma~$decays with the ATLAS detector at the Large Hadron Collider. The analysis uses a proton-proton data sample corresponding to an integrated luminosity of 20.2 fb$^{-1}$ collected at a centre-of-mass energy $\sqrt{s}$ = 8 TeV. Integrated fiducial cross-sections together with normalised differential fiducial cross-sections, sensitive to the kinematics of final-state QED radiation, are obtained. The results are found to be in agreement with state-of-the-art predictions for final-state QED radiation. First measurements of $Z \to ll\gamma\gamma$ decays are also reported.
Unfolded dR distribution for $Z \to \mu\mu\gamma$ process with bare leptons and bkg subtraction. $M_{ll}>20$ GeV. Nexp.un f. = 65362.4 $\pm$ 255.7 , NPowHeg truth =634214.
A search for high-mass charged and neutral bosons decaying to $W\gamma$ and $Z\gamma$ final states is presented in this paper. The analysis uses a data sample of $\sqrt{s} = 13$ TeV proton-proton collisions with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector during LHC Run 2 operation. The sensitivity of the search is determined using models of the production and decay of spin-1 charged bosons and spin-0/2 neutral bosons. The range of resonance masses explored extends from 1.0 TeV to 6.8 TeV. At these high resonance masses, it is beneficial to target the hadronic decays of the $W$ and $Z$ bosons because of their large branching fractions. The decay products of the high-momentum $W/Z$ bosons are strongly collimated and boosted-boson tagging techniques are employed to improve the sensitivity. No evidence of a signal above the Standard Model backgrounds is observed, and upper limits on the production cross-sections of these bosons times their branching fractions to $W\gamma$ and $Z\gamma$ are derived for various boson production models.
The jet mass distribution of large-$R$ jets originating from the hadronic decay of $W$ and $Z$ bosons produced from the decay of BSM bosons with mass $m_X = 2000$ GeV. The decays simulated are for the production models $q\bar{q'}\to X^{\pm} \to W^{\pm}\gamma$ with a spin-1 resonance $X^{\pm}$ and $gg\to X^0 \to Z\gamma$ with a spin-0 resonance $X^{0}$.
Differential and double-differential distributions of kinematic variables of leptons from decays of top-quark pairs ($t\bar{t}$) are measured using the full LHC Run 2 data sample collected with the ATLAS detector. The data were collected at a $pp$ collision energy of $\sqrt{s}=13$ TeV and correspond to an integrated luminosity of 140 fb$^{-1}$. The measurements use events containing an oppositely charged $e\mu$ pair and $b$-tagged jets. The results are compared with predictions from several Monte Carlo generators. While no prediction is found to be consistent with all distributions, a better agreement with measurements of the lepton $p_{\text{T}}$ distributions is obtained by reweighting the $t\bar{t}$ sample so as to reproduce the top-quark $p_{\text{T}}$ distribution from an NNLO calculation. The inclusive top-quark pair production cross-section is measured as well, both in a fiducial region and in the full phase-space. The total inclusive cross-section is found to be \[ \sigma_{t\bar{t}} = 829 \pm 1\;(\textrm{stat}) \pm 13\;(\textrm{syst}) \pm 8\;(\textrm{lumi}) \pm 2\; (\textrm{beam})\ \textrm{pb}, \] where the uncertainties are due to statistics, systematic effects, the integrated luminosity and the beam energy. This is in excellent agreement with the theoretical expectation.
Data bootstrap post unfolding for the differential absolute cross-section for $\textrm{p}_{\textrm{T}}^{e\mu}$. The replicas are obtained by reweighting each observed data event by a random integer generated according to Poisson statistics, using the BootstrapGenerator software package (https://gitlab.cern.ch/atlas-physics/sm/StandardModelTools_BootstrapGenerator/BootstrapGenerator), which implements a technique described in ATL-PHYS-PUB-2021-011 (https://cds.cern.ch/record/2759945). The ATLAS event number and run number of each event are used as seed to uniquely but reproducibly initialise the random number generator for each event. All the provided numbers originate from pseudo-data, including the 0th entry, and are in units of [fb/GeV]. The last bin of the distribution contains the overflow.
New particles with large masses that decay into hadronically interacting particles are predicted by many models of physics beyond the Standard Model. A search for a massive resonance that decays into pairs of dijet resonances is performed using 140 fb$^{-1}$ of proton$-$proton collisions at $\sqrt{s}=13$ TeV recorded by the ATLAS detector during Run 2 of the Large Hadron Collider. Resonances are searched for in the invariant mass of the tetrajet system, and in the average invariant mass of the pair of dijet systems. A data-driven background estimate is obtained by fitting the tetrajet and dijet invariant mass distributions with a four-parameter dijet function and a search for local excesses from resonant production of dijet pairs is performed. No significant excess of events beyond the Standard Model expectation is observed, and upper limits are set on the production cross-sections of new physics scenarios.
The average dijet invariant mass distributions in data, along with the fitted background estimates for 0.28 < $\alpha$ < 0.30.
A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved'' channel) and topologies with boosted final states with hadronic and/or leptonic products partially overlapping and reconstructed as a large-radius jet (``boosted'' channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})<1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos. These constitute the most stringent exclusion limits to date for the model considered.
The $m_{eejj}$ distribution in the resolved electron channel.
We present a search for magnetic monopoles and high-electric-charge objects using LHC Run 2 $\sqrt{s} =$13 TeV proton$-$proton collisions recorded by the ATLAS detector. A total integrated luminosity of 138 fb$^{-1}$ was collected by a specialized trigger. No highly ionizing particle candidate was observed. Considering the Drell-Yan and photon-fusion pair production mechanisms as benchmark models, cross-section upper limits are presented for spin-0 and spin-$\frac{1}{2}$ magnetic monopoles of magnetic charge $1g_\textrm{D}$ and $2g_\textrm{D}$ and for high-electric-charge objects of electric charge $20 \leq |z| \leq 100$, for masses between 200 GeV and 4000 GeV. The search improves by approximately a factor of three the previous cross-section limits on the Drell-Yan production of magnetic monopoles and high-electric charge objects. Also, the first ATLAS limits on the photon-fusion pair production mechanism of magnetic monopoles and high-electric-charge objects have been obtained.
Selection efficiency as a function of transverse kinetic energy $E^\text{kin}_\text{T}=E_\text{kin}\sin\theta$ and pseudorapidity $|\eta|$ for $g=2g_\textrm{D}$ monopoles of mass 2500 GeV.
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.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definitions:</b><br/> <ul> <li> NLEP = 1, either E or MU, PT > 27 GeV, ABS ETA < 2.5 <li> NJETS >= 2, R = 0.4, PT > 26 GeV, ABS ETA < 2.5 <li> NBJETS >= 2 <li> NJETS >= 1, R=1, PT > 355 GeV, ABS ETA < 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/>
Relative differential cross-section as a function of $H_T^{t\bar{t}}$ 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.
A search for leptoquarks decaying into the $b\tau$ final state is performed using Run 2 proton-proton collision data from the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$ at $\sqrt{s} = 13$ TeV recorded by the ATLAS detector. The benchmark models considered in this search are vector leptoquarks with electric charge of 2/3e and scalar leptoquarks with an electric charge of 4/3e. No significant excess above the Standard Model prediction is observed, and 95% confidence level upper limits are set on the cross-section times branching fraction of leptoquarks decaying into $b\tau$. For the vector leptoquark production two models are considered: the Yang-Mills and Minimal coupling models. In the Yang-Mills (Minimal coupling) scenario, vector leptoquarks with a mass below 1.58 (1.35) TeV are excluded for a gauge coupling of 1.0 and below 2.05 (1.99) TeV for a gauge coupling of 2.5. In the case of scalar leptoquarks, masses below 1.28 TeV (1.53 TeV) are excluded for a Yukawa coupling of 1.0 (2.5). Finally, an interpretation of the results with minimal model dependence is performed for each of the signal region categories, and limits on the visible cross-section for beyond the Standard Model processes are provided.
Observed (solid line) and expected (dashed line) 95% CL upper limits for $\lambda$ = 2.5 on the cross-section of singly produced $\widetilde{S_{1}}$ signal hypotheses from the combination of the high b-jet $p_{T}$ category for the $\tau_\text{lep}\tau_\text{had}$ and $\tau_\text{had}\tau_\text{had}$ channels.
A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\varepsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
Observed and expected upper limits at 95% CL on the branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 50 GeV
A measurement of novel event shapes quantifying the isotropy of collider events is performed in 140 fb$^{-1}$ of proton-proton collisions with $\sqrt s=13$ TeV centre-of-mass energy recorded with the ATLAS detector at CERN's Large Hadron Collider. These event shapes are defined as the Wasserstein distance between collider events and isotropic reference geometries. This distance is evaluated by solving optimal transport problems, using the 'Energy-Mover's Distance'. Isotropic references with cylindrical and circular symmetries are studied, to probe the symmetries of interest at hadron colliders. The novel event-shape observables defined in this way are infrared- and collinear-safe, have improved dynamic range and have greater sensitivity to isotropic radiation patterns than other event shapes. The measured event-shape variables are corrected for detector effects, and presented in inclusive bins of jet multiplicity and the scalar sum of the two leading jets' transverse momenta. The measured distributions are provided as inputs to future Monte Carlo tuning campaigns and other studies probing fundamental properties of QCD and the production of hadronic final states up to the TeV-scale.
IRing128 for HT2>=1500 GeV, NJets>=3
IRing128 covariance for HT2>=1500 GeV, NJets>=3 (Table 22)
A search is presented for displaced production of Higgs bosons or $Z$ bosons, originating from the decay of a neutral long-lived particle (LLP) and reconstructed in the decay modes $H\rightarrow \gamma\gamma$ and $Z\rightarrow ee$. The analysis uses the full Run 2 data set of proton$-$proton collisions delivered by the LHC at an energy of $\sqrt{s}=13$ TeV between 2015 and 2018 and recorded by the ATLAS detector, corresponding to an integrated luminosity of 139 fb$^{-1}$. Exploiting the capabilities of the ATLAS liquid argon calorimeter to precisely measure the arrival times and trajectories of electromagnetic objects, the analysis searches for the signature of pairs of photons or electrons which arise from a common displaced vertex and which arrive after some delay at the calorimeter. The results are interpreted in a gauge-mediated supersymmetry breaking model with pair-produced higgsinos that decay to LLPs, and each LLP subsequently decays into either a Higgs boson or a $Z$ boson. The final state includes at least two particles that escape direct detection, giving rise to missing transverse momentum. No significant excess is observed above the background expectation. The results are used to set upper limits on the cross section for higgsino pair production, up to a $\tilde\chi^0_1$ mass of 369 (704) GeV for decays with 100% branching ratio of $\tilde\chi^0_1$ to Higgs ($Z$) bosons for a $\tilde\chi^0_1$ lifetime of 2 ns. A model-independent limit is also set on the production of pairs of photons or electrons with a significant delay in arrival at the calorimeter.
The 95% CL limits on $\sigma(pp \rightarrow \tilde\chi^0_1 \tilde\chi^0_1$) in fb as a function of $\tilde\chi^0_1$ branching ratio to the SM Higgs boson, where the assumed cross-section is for higgsino production, and $\mathcal{B}$($\tilde\chi^0_1$ $\rightarrow Z +\tilde{G}$) = 1 - $\mathcal{B}$($\tilde\chi^0_1$ $\rightarrow H + \tilde{G}$). Several signal hypotheses are overlaid that are labelled by the $\tilde\chi^0_1$ mass, all with a fixed $\tilde\chi^0_1$ lifetime of 2 ns.
A search for a new pseudoscalar $a$-boson produced in events with a top-quark pair, where the $a$-boson decays into a pair of muons, is performed using $\sqrt{s} = 13$ TeV $pp$ collision data collected with the ATLAS detector at the LHC, corresponding to an integrated luminosity of $139\, \mathrm{fb}^{-1}$. The search targets the final state where only one top quark decays to an electron or muon, resulting in a signature with three leptons $e\mu\mu$ and $\mu\mu\mu$. No significant excess of events above the Standard Model expectation is observed and upper limits are set on two signal models: $pp \rightarrow t\bar{t}a$ and $pp \rightarrow t\bar{t}$ with $t \rightarrow H^\pm b$, $H^\pm \rightarrow W^\pm a$, where $a\rightarrow\mu\mu$, in the mass ranges $15$ GeV $ < m_a < 72$ GeV and $120$ GeV $ \leq m_{H^{\pm}} \leq 160$ GeV.
Cutflow for the signal mass point $t\bar{t}a$, $m_{a} = 60$ GeV, as well as the dominant backgrounds estimated from simulation ($t\bar{t}Z$, $WZ$, $t\bar{t}H$) and data, for the corresponding signal mass hypothesis, for the muon channel $\mu\mu\mu$. For the signal yields, a cross section times branching ratio of 1 fb is assumed. The yields are presented before the profile likelihood fit.
This paper reports a search for Higgs boson pair ($hh$) production in association with a vector boson ($W$ or $Z$) using 139 $fb^{-1}$ of proton-proton collision data at $\sqrt{s}=$ 13 TeV recorded with the ATLAS detector at the Large Hadron Collider. The search is performed in final states in which the vector boson decays leptonically ($W\to\ell\nu, Z\to\ell\ell,\nu\nu$ with $\ell=e, \mu$) and the Higgs bosons each decay into a pair of $b$-quarks. It targets $Vhh$ signals from both non-resonant $hh$ production, present in the Standard Model (SM), and resonant $hh$ production, as predicted in some SM extensions. A 95% confidence-level upper limit of 183 (87) times the SM cross-section is observed (expected) for non-resonant $Vhh$ production when assuming the kinematics are as expected in the SM. Constraints are also placed on Higgs boson coupling modifiers. For the resonant search, upper limits on the production cross-sections are derived for two specific models: one is the production of a vector boson along with a neutral heavy scalar resonance $H$, in the mass range 260-1000 GeV, that decays into $hh$, and the other is the production of a heavier neutral pseudoscalar resonance $A$ that decays into a $Z$ boson and $H$ boson, where the $A$ boson mass is 360-800 GeV and the $H$ boson mass is 260-400 GeV. Constraints are also derived in the parameter space of two-Higgs-doublet models.
Data and post-fit signal and background from S+B fit for 315 GeV resonant $H\to 4b$ production in association with a W boson.
Data and post-fit signal and background from S+B fit for 315 GeV resonant $H\to 4b$ production in association with a W boson.
The production of a $W$ boson in association with a single charm quark is studied using 140 $\mathrm{fb}^{-1}$ of $\sqrt{s} = 13\,\mathrm{TeV}$ proton-proton collision data collected with the ATLAS detector at the Large Hadron Collider. The charm quark is tagged by a charmed hadron, reconstructed with a secondary-vertex fit. The $W$ boson is reconstructed from an electron/muon decay and the missing transverse momentum. The mesons reconstructed are $D^{\pm} \to K^\mp \pi^\pm \pi^\pm$ and $D^{*\pm} \to D^{0} \pi^\pm \to (K^\mp \pi^\pm) \pi^\pm$, where $p_{\text{T}}(e, \mu) > 30\,\mathrm{GeV}$, $|\eta(e, \mu)| < 2.5$, $p_{\text{T}}(D) > 8\,\mathrm{GeV}$, and $|\eta(D)| < 2.2$. The integrated and normalized differential cross-sections as a function of the pseudorapidity of the lepton from the $W$ boson decay, and of the transverse momentum of the meson, are extracted from the data using a profile likelihood fit. The measured fiducial cross-sections are $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{-}{+}D^{+}) = 50.2\pm0.2\,\mathrm{(stat.)}\,^{+2.4}_{-2.3}\,\mathrm{(syst.)}\,\mathrm{pb}$, $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{+}{+}D^{-}) = 48.5\pm0.2\,\mathrm{(stat.)}\,^{+2.3}_{-2.2}\,\mathrm{(syst.)}\,\mathrm{pb}$, $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{-}{+}D^{*+}) = 51.1\pm0.4\,\mathrm{(stat.)}\,^{+1.9}_{-1.8}\,\mathrm{(syst.)}\,\mathrm{pb}$, and $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{+}{+}D^{*-}) = 50.0\pm0.4\,\mathrm{(stat.)}\,^{+1.9}_{-1.8}\,\mathrm{(syst.)}\,\mathrm{pb}$. Results are compared with the predictions of next-to-leading-order quantum chromodynamics calculations performed using state-of-the-art parton distribution functions. The ratio of charm to anti-charm production cross-sections is studied to probe the $s$-$\bar{s}$ quark asymmetry and is found to be $R_c^\pm = 0.971\pm0.006\,\mathrm{(stat.)}\pm0.011\,\mathrm{(syst.)}$.
Measured $|\eta(\ell)|$ differential fiducial cross-section times the single-lepton-flavor W boson branching ratio in the $W^{+}+D^{*-}$ channel with the full breakdown of uncertainties.
Jet cross sections were measured in charged current deep inelastic e+-p scattering at high boson virtualities Q^2 with the ZEUS detector at HERA II using an integrated luminosity of 0.36 fb^-1. Differential cross sections are presented for inclusive-jet production as functions of Q^2, Bjorken x and the jet transverse energy and pseudorapidity. The dijet invariant mass cross section is also presented. Observation of three- and four-jet events in charged-current e+-p processes is reported for the first time. The predictions of next-to-leading-order (NLO) QCD calculations are compared to the measurements. The measured inclusive-jet cross sections are well described in shape and normalization by the NLO predictions. The data have the potential to constrain the u and d valence quark distributions in the proton if included as input to global fits.
Differential unpolarized dijet cross section as a function of the dijet mass.
The correlations between flow harmonics $v_n$ for $n=2$, 3 and 4 and mean transverse momentum $[p_\mathrm{T}]$ in $^{129}$Xe+$^{129}$Xe and $^{208}$Pb+$^{208}$Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.44$ TeV and 5.02 TeV, respectively, are measured using charged particles with the ATLAS detector. The correlations are sensitive to the shape and size of the initial geometry, nuclear deformation, and initial momentum anisotropy. The effects from non-flow and centrality fluctuations are minimized, respectively, via a subevent cumulant method and event activity selection based on particle production in the very forward rapidity. The results show strong dependences on centrality, harmonic number $n$, $p_{\mathrm{T}}$ and pseudorapidity range. Current models describe qualitatively the overall centrality- and system-dependent trends but fail to quantitatively reproduce all the data. In the central collisions, where models generally show good agreement, the $v_2$-$[p_\mathrm{T}]$ correlations are sensitive to the triaxiality of the quadruple deformation. The comparison of model to the Pb+Pb and Xe+Xe data suggests that the $^{129}$Xe nucleus is a highly deformed triaxial ellipsoid that is neither a prolate nor an oblate shape. This provides strong evidence for a triaxial deformation of $^{129}$Xe nucleus using high-energy heavy-ion collision.
$\rho_{3}$ Combined_subevent method, for Xe+Xe 5.44 TeV, $|\eta|$<2.5, 0.5< $p_{T}$ <5.0 GeV vs $\Sigma E_{T}$ based Centrality
Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the $b\bar{b}b\bar{b}$, $b\bar{b}\tau^+\tau^-$ and $b\bar{b} \gamma \gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma \gamma$, $ZZ^*$, $WW^*$, $\tau^+ \tau^-$ and $b\bar{b}$ decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton$-$proton collisions at $\sqrt{s}=13$ TeV and correspond to an integrated luminosity of 126$-$139 fb$^{-1}$. The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} < 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4< \kappa_{\lambda}=(\lambda_{HHH}/\lambda_{HHH}^{\textrm{SM}})< 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles. In this relaxed scenario, the constraint becomes $-1.4 < \kappa_{\lambda} < 6.1$ at 95% CL.
Expected constraints in the $\kappa_\lambda$–$\kappa_t$ plane from single-Higgs analyses. The solid lines show the 68% CL contours.
A search for the pair production of heavy leptons as predicted by the type-III seesaw mechanism is presented. The search uses proton-proton collision data at a centre-of-mass energy of 13 TeV, corresponding to 139 fb$^{-1}$ of integrated luminosity recorded by the ATLAS detector during Run 2 of the Large Hadron Collider. The analysis focuses on final states with three or four electrons or muons from the possible decays of new heavy leptons via intermediate electroweak bosons. No significant deviations above the Standard Model expectation are observed; upper and lower limits on the heavy lepton production cross-section and masses are derived respectively. These results are then combined for the first time with the ones already published by ATLAS using the channel with two leptons in the final state. The observed lower limit on the mass of the type-III seesaw heavy leptons combining two, three and four lepton channels together is 910 GeV at the 95% confidence level.
Expected signal and background yields after each of the analysis selection cuts for the 800 GeV mass hypothesis in the Q0-RT CR. Preselection represents events with at least three leptons.
This paper presents results of searches for electroweak production of supersymmetric particles in models with compressed mass spectra. The searches use 139 fb$^{-1}$ of $\sqrt{s}=13$ TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider. Events with missing transverse momentum and two same-flavor, oppositely charged, low transverse momentum leptons are selected, and are further categorized by the presence of hadronic activity from initial-state radiation or a topology compatible with vector-boson fusion processes. The data are found to be consistent with predictions from the Standard Model. The results are interpreted using simplified models of $R$-parity-conserving supersymmetry in which the lightest supersymmetric partner is a neutralino with a mass similar to the lightest chargino, the second-to-lightest neutralino or the slepton. Lower limits on the masses of charginos in different simplified models range from 193 GeV to 240 GeV for moderate mass splittings, and extend down to mass splittings of 1.5 GeV to 2.4 GeV at the LEP chargino bounds (92.4 GeV). Similar lower limits on degenerate light-flavor sleptons extend up to masses of 251 GeV and down to mass splittings of 550 MeV. Constraints on vector-boson fusion production of electroweak SUSY states are also presented.
Number of signal events in SR-S-high for the (m($\tilde{\ell}$),m($\tilde{\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages of selection before and after weighting events to correspond to 140/fb.
Number of signal events in SR-S-high for the (m($\tilde{\ell}$),m($\tilde{\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages of selection before and after weighting events to correspond to 140/fb.
Number of signal events in SR-S-high for the (m($\tilde{\ell}$),m($\tilde{\chi}_{1}^{0}$)) = (150 GeV, 140 GeV) Slepton signal model at different stages of selection before and after weighting events to correspond to 140/fb.
Searches are performed for nonresonant and resonant di-Higgs boson production in the $b\bar{b}\gamma\gamma$ final state. The data set used corresponds to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No excess above the expected background is found and upper limits on the di-Higgs boson production cross sections are set. A 95% confidence-level upper limit of 4.2 times the cross section predicted by the Standard Model is set on $pp \rightarrow HH$ nonresonant production, where the expected limit is 5.7 times the Standard Model predicted value. The expected constraints are obtained for a background hypothesis excluding $pp \rightarrow HH$ production. The observed (expected) constraints on the Higgs boson trilinear coupling modifier $\kappa_{\lambda}$ are determined to be $[-1.5, 6.7]$ $([-2.4, 7.7])$ at 95% confidence level, where the expected constraints on $\kappa_{\lambda}$ are obtained excluding $pp \rightarrow HH$ production from the background hypothesis. For resonant production of a new hypothetical scalar particle $X$ ($X \rightarrow HH \rightarrow b\bar{b}\gamma\gamma$), limits on the cross section for $pp \to X \to HH$ are presented in the narrow-width approximation as a function of $m_{X}$ in the range $251 \leq m_{X} \leq 1000$ GeV. The observed (expected) limits on the cross section for $pp \to X \to HH$ range from 640 fb to 44 fb (391 fb to 46 fb) over the considered mass range.
Comparison of $m_{b\bar{b}}$ distributions when applying the specific b-jet energy calibration and the nominal jet energy calibration. The distributions are fitted using a Bukin function, and the values of the peak position, resolution and the relative improvement are reported in the legend.
Comparison of $m_{b\bar{b}}$ distributions when applying the specific b-jet energy calibration and the nominal jet energy calibration. The distributions are fitted using a Bukin function, and the values of the peak position, resolution and the relative improvement are reported in the legend.
Comparison of $m_{b\bar{b}}$ distributions when applying the specific b-jet energy calibration and the nominal jet energy calibration. The distributions are fitted using a Bukin function, and the values of the peak position, resolution and the relative improvement are reported in the legend.
Measurements of the production cross-sections of the Standard Model (SM) Higgs boson ($H$) decaying into a pair of $\tau$-leptons are presented. The measurements use data collected with the ATLAS detector from $pp$ collisions produced at the Large Hadron Collider at a centre-of-mass energy of $\sqrt{s}=13\,\text{TeV}$, corresponding to an integrated luminosity of $139\,\text{fb}^{-1}$. Leptonic ($\tau\to\ell\nu_{\ell}\nu_{\tau}$) and hadronic ($\tau\to\text{hadrons}~\nu_{\tau}$) decays of the $\tau$-lepton are considered. All measurements account for the branching ratio of $H\to\tau\tau$ and are performed with a requirement $|y_H|<2.5$, where $y_H$ is the true Higgs boson rapidity. The cross-section of the $pp\to H\to\tau\tau$ process is measured to be $2.94 \pm 0.21 \text{(stat)} ^{+\,0.37}_{-\,0.32} \text{(syst)}$ pb, in agreement with the SM prediction of $3.17\pm0.09~ \mbox{pb}$. Inclusive cross-sections are determined separately for the four dominant production modes: $2.65 \pm 0.41 \text{(stat)} ^{+\,0.91}_{-\,0.67} \text{(syst)}$ pb for gluon$-$gluon fusion, $0.197 \pm 0.028 \text{(stat)} ^{+\,0.032}_{-\,0.026} \text{(syst)}$ pb for vector-boson fusion, $0.115 \pm 0.058 \text{(stat)} ^{+\,0.042}_{-\,0.040} \text{(syst)}$ pb for vector-boson associated production, and $0.033 \pm 0.031 \text{(stat)} ^{+\,0.022}_{-\,0.017} \text{(syst)}$ pb for top-quark pair associated production. Measurements in exclusive regions of the phase space, using the simplified template cross-section framework, are also performed. All results are in agreement with the SM predictions.
Observed yields in the VBF_1 signal region category of the lh channel.
Observed yields in the VBF_1 signal region category of the lh channel.
The associated production of a Higgs boson and a top-quark pair is measured in events characterised by the presence of one or two electrons or muons. The Higgs boson decay into a $b$-quark pair is used. The analysed data, corresponding to an integrated luminosity of 139 fb$^{-1}$, were collected in proton-proton collisions at the Large Hadron Collider between 2015 and 2018 at a centre-of-mass energy of $\sqrt{s}=13$ TeV. The measured signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model, is $0.35^{+0.36}_{-0.34}$. This result is compatible with the Standard Model prediction and corresponds to an observed (expected) significance of 1.0 (2.7) standard deviations. The signal strength is also measured differentially in bins of the Higgs boson transverse momentum in the simplified template cross-section framework, including a bin for specially selected boosted Higgs bosons with transverse momentum above 300 GeV.
The ratios $S/B$ (black solid line, referring to the vertical axis on the left) and $S/\sqrt{B}$ (red dashed line, referring to the vertical axis on the right) for each category in the inclusive analysis in the dilepton channel (left) and in the single-lepton channels (right), where $S$ ($B$) is the number of selected signal (background) events predicted by the simulation and normalised to a luminosity of 139 fb$^{-1}$ .
The Standard Model of particle physics describes the known fundamental particles and forces that make up our universe, with the exception of gravity. One of the central features of the Standard Model is a field that permeates all of space and interacts with fundamental particles. The quantum excitation of this field, known as Higgs field, manifests itself as the Higgs boson, the only fundamental particle with no spin. In 2012, a particle with properties consistent with the Higgs boson of the Standard Model was observed by the ATLAS and CMS experiments at the Large Hadron Collider at CERN. Since then, more than 30 times as many Higgs bosons have been recorded by the ATLAS experiment, allowing much more precise measurements and new tests of the theory. Here, on the basis of this larger dataset, we combine an unprecedented number of production and decay processes of the Higgs boson to scrutinize its interactions with elementary particles. Interactions with gluons, photons, and $W$ and $Z$ bosons -- the carriers of the strong, electromagnetic, and weak forces -- are studied in detail. Interactions with three third-generation matter particles (bottom ($b$) and top ($t$) quarks, and tau leptons ($\tau$)) are well measured and indications of interactions with a second-generation particle (muons, $\mu$) are emerging. These tests reveal that the Higgs boson discovered ten years ago is remarkably consistent with the predictions of the theory and provide stringent constraints on many models of new phenomena beyond the Standard Model.
Best-fit values and uncertainties for the cross sections in each measurement region, normalized to the SM predictions for the various parameters. The measurements assume SM branching fractions for all measured decays. The black error bars, blue boxes and yellow boxes show the total, systematic, and statistical uncertainties in the measurements, respectively. The gray bands show the theory uncertainties on the predictions. The level of compatibility between the combined measurement and the SM prediction corresponds to a $p$-value of 94%.
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.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
A search for supersymmetry in events with four or more charged leptons (electrons, muons and $\tau$-leptons) is presented. The analysis uses a data sample corresponding to $139\,\mbox{fb\(^{-1}\)}$ of proton-proton collisions delivered by the Large Hadron Collider at $\sqrt{s}=13$ TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying $\tau$-leptons are designed to target several supersymmetric models, while a general five-lepton signal region targets any new physics phenomena leading to a final state with five charged leptons. Data yields are consistent with Standard Model expectations and results are used to set upper limits on contributions from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of general gauge-mediated supersymmetry, excluding higgsino masses up to $540$ GeV. In $R$-parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of $1.6$ TeV, $1.2$ TeV, and $2.5$ TeV are placed on wino, slepton and gluino masses, respectively.
Expected 95% CL exclusion limits on wino NLSP pair production with RPV LSP decays via $\lambda_{i33}$, where $i \in{1,2}$. The limits are set using the statistical combination of disjoint signal regions. Where two (or more) signal regions overlap, the signal region contributing its observed $\mathrm{CL}_{\mathrm{s}}$ value to the combination is the one with the better (best) expected $\mathrm{CL}_{\mathrm{s}}$ value.
A search for invisible decays of the Higgs boson as well as searches for dark matter candidates, produced together with a leptonically decaying $Z$ boson, are presented. The analysis is performed using proton-proton collisions at a centre-of-mass energy of 13 TeV, delivered by the LHC, corresponding to an integrated luminosity of 139 fb$^{-1}$ and recorded by the ATLAS experiment. Assuming Standard Model cross-sections for $ZH$ production, the observed (expected) upper limit on the branching ratio of the Higgs boson to invisible particles is found to be 19% (19%) at the 95% confidence level. Exclusion limits are also set for simplified dark matter models and two-Higgs-doublet models with an additional pseudoscalar mediator.
Observed lower limit on WIMP-nucleon cross section at 90% CL as a function of m(WIMP), assuming Higgs-portal scenario with Majorana WIMP.
A search for R-parity violating supersymmetry in final states characterised by high jet multiplicity, at least one isolated light lepton and either zero or at least three $b$-tagged jets is presented. The search uses 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data collected by the ATLAS experiment during Run 2 of the Large Hadron Collider. The results are interpreted in the context of R-parity-violating supersymmetry models that feature gluino production, top-squark production, or electroweakino production. The dominant sources of background are estimated using a data-driven model, based on observables at medium jet multiplicity, to predict the $b$-tagged jet multiplicity distribution at the higher jet multiplicities used in the search. Machine learning techniques are used to reach sensitivity to electroweakino production, extending the data-driven background estimation to the shape of the machine learning discriminant. No significant excess over the Standard Model expectation is observed and exclusion limits at the 95% confidence-level are extracted, reaching as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark mass, and 320 (365) GeV in higgsino (wino) mass.
The observed data event yields and the corresponding estimates for the backgrounds in the different $b$-jet multiplicity bins for the 60 GeV jet $p_{\mathrm{T}}$ threshold region in the $1\ell$ category for at least 11 jets. The background is estimated by including all bins in the fit. All uncertainties, which may be correlated across the bins, are included in the total background uncertainty.
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb$^{-1}$ is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain $b$-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26$^{+17}_{-15}$ fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24$^{+7}_{-6}$ fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0$\pm$2.4 fb.
Comparison between data and prediction for the distribution of b-jets multiplicity in the 2LOS,$\geq$6j,$\geq$3b region after the fit.
The results of a search for direct pair production of top squarks and for dark matter in events with two opposite-charge leptons (electrons or muons), jets and missing transverse momentum are reported, using 139 fb$^{-1}$ of integrated luminosity from proton-proton collisions at $\sqrt{s} = 13$ TeV, collected by the ATLAS detector at the Large Hadron Collider during Run 2 (2015-2018). This search considers the pair production of top squarks and is sensitive across a wide range of mass differences between the top squark and the lightest neutralino. Additionally, spin-0 mediator dark-matter models are considered, in which the mediator is produced in association with a pair of top quarks. The mediator subsequently decays to a pair of dark-matter particles. No significant excess of events is observed above the Standard Model background, and limits are set at 95% confidence level. The results exclude top squark masses up to about 1 TeV, and masses of the lightest neutralino up to about 500 GeV. Limits on dark-matter production are set for scalar (pseudoscalar) mediator masses up to about 250 (300) GeV.
Two-body selection acceptance (a) SR-SF$^{2-body}_{[110,120)}$, (b) SR-SF1$^{2-body}_{[120,140)}$, (c) SR-SF2$^{2-body}_{[140,160)}$, (d) SR-SF3$^{2-body}_{[160,180)}$, (e) SR-SF4$^{2-body}_{[180,220)}$, (f) SR-SF5$^{2-body}_{[220,\infty)}$ for a simplified model assuming $ \tilde{t}_1$ pair production.
Two-body selection acceptance (a) SR-SF$^{2-body}_{[110,120)}$, (b) SR-SF1$^{2-body}_{[120,140)}$, (c) SR-SF2$^{2-body}_{[140,160)}$, (d) SR-SF3$^{2-body}_{[160,180)}$, (e) SR-SF4$^{2-body}_{[180,220)}$, (f) SR-SF5$^{2-body}_{[220,\infty)}$ for a simplified model assuming $ \tilde{t}_1$ pair production.
Two-body selection acceptance (a) SR-SF$^{2-body}_{[110,120)}$, (b) SR-SF1$^{2-body}_{[120,140)}$, (c) SR-SF2$^{2-body}_{[140,160)}$, (d) SR-SF3$^{2-body}_{[160,180)}$, (e) SR-SF4$^{2-body}_{[180,220)}$, (f) SR-SF5$^{2-body}_{[220,\infty)}$ for a simplified model assuming $ \tilde{t}_1$ pair production.
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV $<p_T<$ 2.5 TeV and pseudorapidity $|\eta| < 2.1$ from an integrated luminosity of 33 fb$^{-1}$ of $\sqrt{s}=13$ TeV proton-proton collisions are reconstructed with the ATLAS detector at the Large Hadron Collider. Charged-particle tracks with $p_T > 500$ MeV and $|\eta| < 2.5$ are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet $p_T$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations.
$n_{ch}$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.
$n_{ch}$ , 1000 GeV < Jet p_{T} < 1200 GeV, both jets.
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.
Measured cross sections for isolated-photon plus two-jet production as functions of $\Delta y^{\gamma-\textrm{jet}}$ for the direct-enriched phase-space. The predictions from Sherpa NLO are also included.
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.
The normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ 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 normalised parton-level differential cross-section measured in the fiducial phase-space as a function of the $|\Delta \phi (t\bar{t}, Z)|/\pi$ in the 4$\ell$ 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.
Studies of the fragmentation of jets into charged particles in heavy-ion collisions can provide information about the mechanism of jet-quenching by the hot and dense QCD matter created in such collisions, the quark-gluon plasma. This paper presents a measurement of the angular distribution of charged particles around the jet axis in $\sqrt{s_{\mathrm{NN}}}=$ 5.02 TeV Pb+Pb and $pp$ collisions, using the ATLAS detector at the LHC. The Pb+Pb and $pp$ data sets have integrated luminosities of 0.49 nb$^{-1}$ and 25 pb$^{-1}$, respectively. The measurement is performed for jets reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R = 0.4$ and is extended to an angular distance of $r= 0.8$ from the jet axis. Results are presented as a function of Pb+Pb collision centrality and distance from the jet axis for charged particles with transverse momenta in the 1$-$63 GeV range, matched to jets with transverse momenta in the 126$-$316 GeV range and an absolute value of jet rapidity of less than 1.7. Modifications to the measured distributions are quantified by taking a ratio to the measurements in $pp$ collisions. Yields of charged particles with transverse momenta below 4 GeV are observed to be increasingly enhanced as a function of angular distance from the jet axis, reaching a maximum at $r=0.6$. Charged particles with transverse momenta above 4 GeV have an enhanced yield in Pb+Pb collisions in the jet core for angular distances up to $r = 0.05$ from the jet axis, with a suppression at larger distances.
D(pT,r)_PbPb The charged particle distributions around jets as a function of distance from the jet axis in PbPb collisions at 5.02 TeV for different centrality, track pT and jet pT ranges.
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.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definition:</b><br/> <ul> <li> NLEP = 0, either E or MU, PT > 15 GeV, ABS ETA < 1.37 <li> NJETS >= 6, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 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/>
Covariance matrix of the relative differential cross-section as function of $p_{T}^{t,1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.
Jet substructure quantities are measured using jets groomed with the soft-drop grooming procedure in dijet events from 32.9 fb$^{-1}$ of $pp$ collisions collected with the ATLAS detector at $\sqrt{s} = 13$ TeV. These observables are sensitive to a wide range of QCD phenomena. Some observables, such as the jet mass and opening angle between the two subjets which pass the soft-drop condition, can be described by a high-order (resummed) series in the strong coupling constant $\alpha_S$. Other observables, such as the momentum sharing between the two subjets, are nearly independent of $\alpha_S$. These observables can be constructed using all interacting particles or using only charged particles reconstructed in the inner tracking detectors. Track-based versions of these observables are not collinear safe, but are measured more precisely, and universal non-perturbative functions can absorb the collinear singularities. The unfolded data are directly compared with QCD calculations and hadron-level Monte Carlo simulations. The measurements are performed in different pseudorapidity regions, which are then used to extract quark and gluon jet shapes using the predicted quark and gluon fractions in each region. All of the parton shower and analytical calculations provide an excellent description of the data in most regions of phase space.
Data from FigAux 21b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
Data from FigAux 21b. The unfolded charged-particle $log_{10}(\rho^2)$ distribution for the more central of the two anti-kt R=0.8 jets with $p_T$ > 300 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data. The distributions are normalized to the integrated cross section, $\sigma$(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$.
This paper presents a search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudoscalar mediator, $a$, which decays into the dark-matter particles. Processes where the pseudoscalar mediator is produced in association with a single top quark in the 2HDM+$a$ model are explored for the first time at the LHC. Several final states which include either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum are considered. The analysis is based on proton-proton collision data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run2 (2015-2018), corresponding to an integrated luminosity of 139 fb$^{-1}$. No significant excess above the Standard Model predictions is found. The results are expressed as 95% confidence-level limits on the parameters of the signal models considered.
The observed exclusion contours as a function of $(m_a, m_{H^{\pm}})$, assuming only $tW$+DM contributions, for the tW2L analysis channel.
A search for heavy neutral Higgs bosons is performed using the LHC Run 2 data, corresponding to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=13$ TeV recorded with the ATLAS detector. The search for heavy resonances is performed over the mass range 0.2-2.5 TeV for the $\tau^+\tau^-$ decay with at least one $\tau$-lepton decaying into final states with hadrons. The data are in good agreement with the background prediction of the Standard Model. In the $M_{h}^{125}$ scenario of the Minimal Supersymmetric Standard Model, values of $\tan\beta>8$ and $\tan\beta>21$ are excluded at the 95% confidence level for neutral Higgs boson masses of 1.0 TeV and 1.5 TeV, respectively, where $\tan\beta$ is the ratio of the vacuum expectation values of the two Higgs doublets.
Expected 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of the scalar boson mass and the fraction of the b-associated production. The limits are calculated from a statistical combination of the 1l1tau_h and 2tau_h channels.
Expected 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of the scalar boson mass and the fraction of the b-associated production. The limits are calculated from a statistical combination of the 1l1tau_h and 2tau_h channels.
Expected 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of the scalar boson mass and the fraction of the b-associated production. The limits are calculated from a statistical combination of the 1l1tau_h and 2tau_h channels.
A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of $\sqrt{s} = $13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing $b$-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical $Z'$ bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross-sections, the $Z'$ boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1$-$3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 TeV to 0.9 TeV and from 2.0 TeV to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.
Expected and observed upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 1 TeV.
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.
- - - - - - - - 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 > 27 GeV, ABS ETA < 2.5 <li> NJETS >= 4, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 2 </ul><br/> <i>Boosted:</i> <ul> <li> NLEP = 1, either E or MU, PT > 27 GeV, ABS ETA < 2.5 <li> NJETS >= 1, R = 0.4, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 1 <li> NJETS >= 1, R=1, PT > 350 GeV, ABS ETA < 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/>
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
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.
The statistical correlation matrix of all the absolute differential cross-sections measured in the fiducial phase-space in the electron-muon channel.
The inclusive top quark pair ($t\bar{t}$) production cross-section $\sigma_{t\bar{t}}$ has been measured in proton$-$proton collisions at $\sqrt{s}=13$ TeV, using $36.1$ fb$^{-1}$ of data collected in 2015$-$16 by the ATLAS experiment at the LHC. Using events with an opposite-charge $e\mu$ pair and $b$-tagged jets, the cross-section is measured to be: \begin{equation}\nonumber \sigma_{t\bar{t}} = 826.4 \pm 3.6\,\mathrm{(stat)}\ \pm 11.5\,\mathrm{(syst)}\ \pm 15.7\,\mathrm{(lumi)}\ \pm 1.9\,\mathrm{(beam)}\,\mathrm{pb}, \end{equation} where the uncertainties reflect the limited size of the data sample, experimental and theoretical systematic effects, the integrated luminosity, and the LHC beam energy, giving a total uncertainty of 2.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. It is used to determine the top quark pole mass via the dependence of the predicted cross-section on $m_t^{\mathrm{pole}}$, giving $m_t^{\mathrm{pole}}=173.1^{+2.0}_{-2.1}$ GeV. It is also combined with measurements at $\sqrt{s}=7$ TeV and $\sqrt{s}=8$ TeV to derive ratios and double ratios of $t\bar{t}$ and $Z$ cross-sections at different energies. The same event sample is used to measure absolute and normalised differential cross-sections as functions of single-lepton and dilepton kinematic variables, and the results compared with predictions from various Monte Carlo event generators.
Normalised differential cross-section in the fiducial region as a function of the azimuthal angle between the leptons and dilepton invariant mass. The first four columns give the cross-section including contributions from leptonic tau decays in the four mass bins, and the last four columns do not include the leptonic tau contributions. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).
A test of CP invariance in Higgs boson production via vector-boson fusion is performed in the $H\rightarrow\tau\tau$ decay channel. This test uses the Optimal Observable method and is carried out using 36.1 $\mathrm{fb}^{-1}$ of $\sqrt{s}$ = 13 TeV proton$-$proton collision data collected by the ATLAS experiment at the LHC. Contributions from CP-violating interactions between the Higgs boson and electroweak gauge bosons are described by an effective field theory, in which the parameter $\tilde{d}$ governs the strength of CP violation. No sign of CP violation is observed in the distributions of the Optimal Observable, and $\tilde{d}$ is constrained to the interval $[-0.090, 0.035]$ at the 68% confidence level (CL), compared to an expected interval of $\tilde{d} \in [-0.035,0.033]$ based upon the Standard Model prediction. No constraints can be set on $\tilde{d}$ at 95% CL, while an expected 95% CL interval of $\tilde{d} \in [-0.21,0.15]$ for the Standard Model hypothesis was expected.
Post-fit BDT distributions in the $Z\to \ell\ell$ CR for the $\tau_{\mathrm{lep}}\tau_{\mathrm{lep}}$ SF analysis channel. The size of the combined statistical, experimental, and theoretical uncertainties is given. The exact value of the $p_{\mathrm{T}}$ cut on the leptons depends on the trigger.
The azimuthal anisotropy of charged particles produced in $\sqrt{s_{\mathrm{NN}}}=8.16$ TeV $p$+Pb collisions is measured with the ATLAS detector at the LHC. The data correspond to an integrated luminosity of $165$ $\mathrm{nb}^{-1}$ that was collected in 2016. Azimuthal anisotropy coefficients, elliptic $v_2$ and triangular $v_3$, extracted using two-particle correlations with a non-flow template fit procedure, are presented as a function of particle transverse momentum ($p_\mathrm{T}$) between $0.5$ and $50$ GeV. The $v_2$ results are also reported as a function of centrality in three different particle $p_\mathrm{T}$ intervals. The results are reported from minimum-bias events and jet-triggered events, where two jet $p_\mathrm{T}$ thresholds are used. The anisotropies for particles with $p_\mathrm{T}$ less than about $2$ GeV are consistent with hydrodynamic flow expectations, while the significant non-zero anisotropies for $p_\mathrm{T}$ in the range $9$-$50$ GeV are not explained within current theoretical frameworks. In the $p_\mathrm{T}$ range $2$-$9$ GeV, the anisotropies are larger in minimum-bias than in jet-triggered events. Possible origins of these effects, such as the changing admixture of particles from hard scattering and the underlying event, are discussed.
Distribution of relative HS-UE pair fractions from $p_{T}^{jet}>75$ GeV events plotted as a function of A-particle $p_\mathrm{T}$ for 0-5% centrality.
This paper reports on a search for heavy resonances decaying into $WW$, $ZZ$ or $WZ$ using proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV. The data, corresponding to an integrated luminosity of 139 $\mathrm{fb^{-1}}$, were recorded with the ATLAS detector from 2015 to 2018 at the Large Hadron Collider. The search is performed for final states in which one $W$ or $Z$ boson decays leptonically, and the other $W$ boson or $Z$ boson decays hadronically. The data are found to be described well by expected backgrounds. Upper bounds on the production cross sections of heavy scalar, vector or tensor resonances are derived in the mass range 300-5000 GeV within the context of Standard Model extensions with warped extra dimensions or including a heavy vector triplet. Production through gluon-gluon fusion, Drell-Yan or vector-boson fusion are considered, depending on the assumed model.
Upper 95% CLs limits on the ggF production cross section of Gravitons in their $ZZ$ decays as a function of the resonance mass.
To assess the properties of the quark-gluon plasma formed in heavy-ion collisions, the ATLAS experiment at the LHC measures a correlation between the mean transverse momentum and the magnitudes of the flow harmonics. The analysis uses data samples of lead-lead and proton-lead collisions obtained at the centre-of-mass energy per nucleon pair of 5.02 TeV, corresponding to total integrated luminosities of $22 ~\mu b^{-1}$ and $28~nb^{-1}$, respectively. The measurement is performed using a modified Pearson correlation coefficient with the charged-particle tracks on an event-by-event basis. The modified Pearson correlation coefficients for the $2^{nd}$-, 3$^{rd}$-, and 4$^{th}$-order harmonics are measured as a function of event centrality quantified as the number of charged particles or the number of nucleons participating in the collision. The measurements are performed for several intervals of the charged-particle transverse momentum. The correlation coefficients for all studied harmonics exhibit a strong centrality evolution in the lead-lead collisions, which only weakly depends on the charged-particle momentum range. In the proton-lead collisions, the modified Pearson correlation coefficient measured for the second harmonics shows only weak centrality dependence. The data is qualitatively described by the predictions based on the hydrodynamical model.
The $cov(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.
A search is presented for pair-production of long-lived neutral particles using 33 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data, collected during 2016 by the ATLAS detector at the LHC. This search focuses on a topology in which one long-lived particle decays in the ATLAS inner detector and the other decays in the muon spectrometer. Special techniques are employed to reconstruct the displaced tracks and vertices in the inner detector and in the muon spectrometer. One event is observed that passes the full event selection, which is consistent with the estimated background. Limits are placed on scalar boson propagators with masses from 125 GeV to 1000 GeV decaying into pairs of long-lived hidden-sector scalars with masses from 8 GeV to 400 GeV. The limits placed on several low-mass scalars extend previous exclusion limits in the range of proper lifetimes $c \tau$ from 5 cm to 1 m.
The impact of the IDVx selections on the selection efficiency for the MC signal sample with a $\Phi$ with a mass of 400 GeV decaying to an LLP with a mass of 50 GeV.
The production cross-sections for $W^{\pm}$ and $Z$ bosons are measured using ATLAS data corresponding to an integrated luminosity of 4.0 pb$^{-1}$ collected at a centre-of-mass energy $\sqrt{s}=2.76$ TeV. The decay channels $W \rightarrow \ell \nu$ and $Z \rightarrow \ell \ell $ are used, where $\ell$ can be an electron or a muon. The cross-sections are presented for a fiducial region defined by the detector acceptance and are also extrapolated to the full phase space for the total inclusive production cross-section. The combined (average) total inclusive cross-sections for the electron and muon channels are: \begin{eqnarray} \sigma^{\text{tot}}_{W^{+}\rightarrow \ell \nu}& = & 2312 \pm 26\ (\text{stat.})\ \pm 27\ (\text{syst.}) \pm 72\ (\text{lumi.}) \pm 30\ (\text{extr.})\text{pb} \nonumber, \\ \sigma^{\text{tot}}_{W^{-}\rightarrow \ell \nu}& = & 1399 \pm 21\ (\text{stat.})\ \pm 17\ (\text{syst.}) \pm 43\ (\text{lumi.}) \pm 21\ (\text{extr.})\text{pb} \nonumber, \\ \sigma^{\text{tot}}_{Z \rightarrow \ell \ell}& = & 323.4 \pm 9.8\ (\text{stat.}) \pm 5.0\ (\text{syst.}) \pm 10.0\ (\text{lumi.}) \pm 5.5 (\text{extr.}) \text{pb} \nonumber. \end{eqnarray} Measured ratios and asymmetries constructed using these cross-sections are also presented. These observables benefit from full or partial cancellation of many systematic uncertainties that are correlated between the different measurements.
Measured fiducial cross-section ratio R_{W+/W-} = sigma (W+ -> l+ nu) / sigma (W- -> l- nubar) where l = e, mu.
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