We present a measurement of the forward--backward asymmetry in top quark-antiquark production using the full Tevatron Run II dataset collected by the D0 experiment at Fermilab. The measurement is performed in lepton+jets final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be 10.6+-3.0 %. Results are consistent with the standard model predictions which range from 5.0% to 8.8%. We also present the dependence of the asymmetry on the invariant mass of the top quark--antiquark system and the difference in rapidities of top quark and antiquark.
Production-level forward-backward asymmetry as a function of the absolute difference in rapidity of the top quark and antiquark. The measured values are calibrated and listed with their total uncertainties. The theoretical predictions are based on MC@NLO simulation.
Production-level forward-backward asymmetry as a function of the invariant mass of the top quark-antiquark system. The measured values are calibrated and listed with their total uncertainties. The theoretical predictions are based on MC@NLO simulation.
This report describes the first search for top squark pair production in the channel stop_1 stopbar_1 -> b bbar chargino_1 chargino_1 -> ee+jets+MEt using 74.9 +- 8.9 pb~-1 of data collected using the D0 detector. A 95% confidence level upper limit on sigma*B is presented. The limit is above the theoretical expectation for sigma*B for this process, but does show the sensitivity of the current D0 data set to a particular topology for new physics.
Data are extracted from the figure. Sigma*Br.
We present a measurement of tbar-t production using multijet final states in pbar-p collisions at a center-of-mass energy of 1.8 TeV, with an integrated luminosity of 110.3 pb(-1). The analysis has been optimized using neural networks to achieve the smallest expected fractional uncertainty on the tbar-t production cross section, and yields a cross section of 7.1 +/- 2.8(stat.) +/- 1.5(syst.) pb, assuming a top quark mass of 172.1 GeV/c^(2). Combining this result with previous D0 measurements, where one or both of the W bosons decay leptonically, gives a tbar-t production cross section of 5.9 +/- 1.2(stat) +/- 1.1(syst) pb.
No description provided.
We have studied tbar-t production using multijet final states in pbar-p collisions at a center-of-mass energy of 1.8 TeV, with an integrated luminosity of 110.3 pb(-1). Each of the top quarks with these final states decays exclusively to a bottom quark and a W boson, with the W bosons decaying into quark-antiquark pairs. The analysis has been optimized using neural networks to achieve the smallest expected fractional uncertainty on the tbar-t production cross section, and yields a cross section of 7.1 +/- 2.8(stat.) +/- 1.5(syst.) pb, assuming a top quark mass of 172.1 GeV/c^(2). Combining this result with previous D0 measurements, where one or both of the W bosons decay leptonically, gives a tbar t production cross section of 5.9 +/- 1.2(stat) +/- 1.1(syst) pb.
The second value is the combination of the data reported here combined withthe previous result of D0 reported in PRL 79(1997)1203.
We determine the top quark mass m_t using t-tbar pairs produced in the D0 detector by \sqrt{s} = 1.8 TeV p-pbar collisions in a 125 pb^-1 exposure at the Fermilab Tevatron. We make a two constraint fit to m_t in t-tbar -> b W^+bbar W^- final states with one W boson decaying to q-qbar and the other to e-nu or mu-nu. Likelihood fits to the data yield m_t(l+jets) = 173.3 +- 5.6 (stat) +- 5.5 (syst) GeV/c^2. When this result is combined with an analysis of events in which both W bosons decay into leptons, we obtain m_t = 172.1 +- 5.2 (stat) +- 4.9 (syst) GeV/c^2. An alternate analysis, using three constraint fits to fixed top quark masses, gives m_t(l+jets) = 176.0 +- 7.9 (stat) +- 4.8 (syst) GeV/C^2, consistent with the above result. Studies of kinematic distributions of the top quark candidates are also presented.
No description provided.
We present a measurement of the ttbar production cross section in ppbar collisions at root(s) = 1.8TeV by the D0 experiment at the Fermilab Tevatron. The measurement is based on data from an integrated luminosity of approximately 125 pb~-1 accumulated during the 1992-1996 collider run. We observe 39 ttbar candidate events in the dilepton and lepton+jets decay channels with an expected background of 13.7+-2.2 events. For a top quark mass of 173.3GeV/c~2, we measure the ttbar production cross section to be 5.5+-1.8 pb.
Different channels are used for evaluation of the cross section magnitudes. The last value is obtained from the previous one by adding the errors in quadrature.
The DO collaboration reports on a search for the Standard Model top quark in pbar-p collisions at Sqrt(s)=1.8TeV at the Fermilab Tevatron, with an integrated luminosity of approximately 50pb-1. We have searched for t-tbar production in the dilepton and single-lepton decay channels, with and without tagging of b-quark jets. We observed 17 events with an expected background of 3.8+/-0.6 events. The probability for an upward fluctuation of the background to produce the observed signal is 2.0E-6 (equivalent to 4.6 standard deviations). The kinematic properties of the excess events are consistent with top quark decay. We conclude that we have observed the top quark and measure its mass to be 199~+19_21 (stat.)+/- 22 (syst.)GeV/c**2 and its production cross section to be 6.4 +/- 2.2 pb.
Cross section refers to top quark mass equal 199. (+19, -21, +- 22) GeV.
We present a search for electroweak production of single top quarks in $\approx 90$ $pb^{-1}$ of data collected with the DZero detector at the Fermilab Tevatron collider. Using arrays of neural networks to separate signals from backgrounds, we set upper limits on the cross sections of 17 pb for the s-channel process $p\bar{p} \to tb + X$, and 22 pb for the t-channel process $p\bar{p} \to tqb + X$, both at the 95% confidence level.
No description provided.
We present a search for electroweak production of single top quarks in the electron+jets and muon+jets decay channels. The measurements use ~90 pb^-1 of data from Run 1 of the Fermilab Tevatron collider, collected at 1.8 TeV with the DZero detector between 1992 and 1995. We use events that include a tagging muon, implying the presence of a b jet, to set an upper limit at the 95% confidence level on the cross section for the s-channel process ppbar->tb+X of 39 pb. The upper limit for the t-channel process ppbar->tqb+X is 58 pb.
No description provided.
None
The cross section was obtained aunder the assumption that top quark has a mass of 200 GeV.
We present the first model-independent measurement of the helicity of $W$ bosons produced in top quark decays, based on a 1 fb$^{-1}$ sample of candidate $t\bar{t}$ events in the dilepton and lepton plus jets channels collected by the D0 detector at the Fermilab Tevatron $p\bar{p}$ Collider. We reconstruct the angle $\theta^*$ between the momenta of the down-type fermion and the top quark in the $W$ boson rest frame for each top quark decay. A fit of the resulting \costheta distribution finds that the fraction of longitudinal $W$ bosons $f_0 = 0.425 \pm 0.166 \hbox{(stat.)} \pm 0.102 \hbox{(syst.)}$ and the fraction of right-handed $W$ bosons $f_+ = 0.119 \pm 0.090 \hbox{(stat.)} \pm 0.053 \hbox{(syst.)}$, which is consistent at the 30% C.L. with the standard model.
COS(THETA*) distribution for leptonic W decay in lepton+jets events.. Data are read from plots and errors are statistcial (sqrt(N)).
COS(THETA*) distribution for hadronic W decay in lepton+jets events.. Data are read from plots and errors are statistcial (sqrt(N)).
COS(THETA*) distribution for W decay in dilepton events.. Data are read from plots and errors are statistcial (sqrt(N)).
We present a measurement of the differential cross section for $t\bar{t}$ events produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of the transverse momentum ($p_T$) of the top quark. The selected events contain a high-$p_T$ lepton ($\ell$), four or more jets, and a large imbalance in $p_T$, and correspond to 1 fb${}^{-1}$ of integrated luminosity recorded with the D0 detector. Each event must have at least one candidate for a $b$ jet. Objects in the event are associated through a constrained kinematic fit to the $t\bar{t}\to WbW\bar{b} \to \ell\nu b q\bar{q}'\bar{b}$ process. Results from next-to-leading-order perturbative QCD calculations agree with the measured differential cross section. Comparisons are also provided to predictions from Monte Carlo event generators using QCD calculations at different levels of precision.
Total cross section for TOP TOPBAR production integrating over PT.
The inclusive PT spectra for TOP TOPBAR production.
We report the first observation of single-top-quark production in the s channel through the combination of the CDF and D0 measurements of the cross section in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV. The data correspond to total integrated luminosities of up to 9.7 fb-1 per experiment. The measured cross section is $\sigma_s = 1.29^{+0.26}_{-0.24}$ pb. The probability of observing a statistical fluctuation of the background to a cross section of the observed size or larger is $1.8 \times 10^{-10}$, corresponding to a significance of 6.3 standard deviations for the presence of an s-channel contribution to the production of single-top quarks.
The measured cross section of single-top-quark production in the s channel.
A search is presented for the pair production of light scalar top quarks in sqrt(s) = 7 TeV proton-proton collisions recorded with the ATLAS detector at the Large Hadron Collider. This analysis uses the full data sample collected during 2011 that corresponds to a total integrated luminosity of 4.7 fb-1. Light scalar top quarks are searched for in events with two opposite-sign leptons (e, mu), large missing transverse momentum and at least one jet in the final state. No excess over Standard Model expectations is found, and the results are interpreted under the assumption that the light scalar top decays to a b-quark in addition to an on-shell chargino whose decay occurs through a virtual W boson. If the chargino mass is 106 GeV, light scalar top quark masses up to 130 GeV are excluded for neutralino masses below 70 GeV.
Distribution of the PT of the leading electron for E-E events in the Signal Region, before the application of the leading lepton PT cut.
Distribution of the PT of the leading muon for MU-MU events in the Signal Region, before the application of the leading lepton PT cut.
Distribution of the PT of the leading electron for E-MU events in the Signal Region, before the application of the leading lepton PT cut.
The results of a search for direct pair production of heavy top-quark partners in 4.7 fb-1 of integrated luminosity from pp collisions at sqrt(s) = 7 TeV collected by the ATLAS detector at the LHC are reported. Heavy top-quark partners decaying into a top quark and a neutral non-interacting particle are searched for in events with two leptons in the final state. No excess above the Standard Model expectation is observed. Limits are placed on the mass of a supersymmetric scalar top and of a spin-1/2 top-quark partner. A spin-1/2 top-quark partner with a mass between 300 GeV and 480 GeV, decaying to a top quark and a neutral non-interacting particle lighter than 100 GeV, is excluded at 95% confidence level.
(1) Number of generated MC events for the scalar top signal grid (2) Relative Cross section uncertainties for the scalar top signal grid.
(1) Acceptance of the same flavour selection for the scalar top signal grid (2) Selection efficiency of the same flavour selection for the scalar top signal grid (3) Product of the acceptance and efficiency of the same flavour selection for the scalar top signal grid (4) Relative experimental uncertainties on the acceptance times efficiency of the same flavour selection for the scalar top signal grid.
(1) Acceptance of the different flavour selection for the scalar top signal grid (2) Selection efficiency of the different flavour selection for the scalar top signal grid (3) Product of the acceptance and efficiency of the different flavour selection for the scalar top signal grid (4) Relative experimental uncertainties on the acceptance times efficiency of the different flavour selection for the scalar top signal grid.
A search is presented for direct top squark pair production in final states with one isolated electron or muon, jets, and missing transverse momentum in proton-proton collisions at sqrt(s) = 7 TeV. The measurement is based on 4.7 fb-1 of data collected with the ATLAS detector at the LHC. Each top squark is assumed to decay to a top quark and the lightest supersymmetric particle (LSP). The data are found to be consistent with Standard Model expectations. Top squark masses between 230 GeV and 440 GeV are excluded with 95% confidence for massless LSPs, and top squark masses around 400 GeV are excluded for LSP masses up to 125 GeV.
The observed and standard model prediction for the distribution of missing ET in signal region A.
The observed 95% exclusion limits for the five signal regions.
The expected 95% exclusion limits for the five signal regions.
This letter reports the results of a search for top and bottom squarks from gluino pair production in 4.7 fb^-1 of pp collisions at sqrt(s) = 7 TeV using the ATLAS detector at the LHC. The search is performed in events with large missing transverse momentum and at least three jets identified as originating from a b-quark. Exclusion limits are presented for a variety of gluino-mediated models with gluino masses up to 1 TeV excluded.
Figure 2-a. Observed limit +1sigma-th.
Figure 2-a. Observed limit.
Figure 2-a. Observed limit -1sigma-th.
This paper presents a search for a new heavy particle produced in association with a top or antitop quark. Two models in which the new heavy particle is a color singlet or a color triplet are considered, decaying respectively to tbarq or tq, leading to a resonance within the ttbar + jets signature. The full 2011 ATLAS pp collision dataset from the LHC (4.7 fb-1) is used to search for ttbar events produced in association with jets, in which one of the W bosons from the top quarks decays leptonically and the other decays hadronically. The data are consistent with the Standard Model expectation, and a new particle with mass below 430 GeV for both W boson and color triplet models is excluded at 95% confidence level, assuming unit right-handed coupling.
Upper limits of the cross sections and couling (g_R) in the WPRIME colour singlet model.
Upper limits of the cross sections and couling (g_R) in the PHI colour triplet model.
A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3fb-1 of pp collision data at sqrt(s)=8TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
Distribution of mT2 for events passing all the signal candidate selection requirements, except that on mT2 of the L90 and L120 selections, for SF events.
Distribution of mT2 for events passing all the signal candidate selection requirements, except that on mT2 of the L90 and L120 selections, for DF events.
Distribution of mT2 for events passing all the signal candidate selection requirements, except that on mT2 of the L100 selection, for SF events.
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of $20.1 \rm{fb}^{-1}$ of proton-proton collision data at $\sqrt{s}=8$ TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via $\tilde{t} \rightarrow t \tilde{\chi}_{1}^{0}$ or $\tilde{t}\rightarrow b\tilde{\chi}_{1}^{\pm} \rightarrow b W^{\left(\ast\right)} \tilde{\chi}_{1}^{0}$, where $\tilde{\chi}_{1}^{0}$ ($\tilde{\chi}_{1}^{\pm}$) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of $\tilde{t} \rightarrow t \tilde{\chi}_{1}^{0}$. For a branching fraction of 100%, top squark masses in the range 270-645 GeV are excluded for $\tilde{\chi}_{1}^{0}$ masses below 30 GeV. For a branching fraction of 50% to either $\tilde{t} \rightarrow t \tilde{\chi}_{1}^{0}$ or $\tilde{t}\rightarrow b\tilde{\chi}_{1}^{\pm}$, and assuming the $\tilde{\chi}_{1}^{\pm}$ mass to be twice the $\tilde{\chi}_{1}^{0}$ mass, top squark masses in the range 250-550 GeV are excluded for $\tilde{\chi}_{1}^{0}$ masses below 60 GeV.
Etmiss distribution for SRA1 and SRA2 after all selection requirements except those on Etmiss.
Etmiss distribution for SRA3 and SRA4 after all selection requirements except those on Etmiss.
Etmiss distribution for SRB after all selection requirements except those on Etmiss.
The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton--proton collision data at $\sqrt{s} = 8$ TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of $20$ fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay modes considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a $W$ boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the $W$ bosons or the top quarks are off-shell. Decay modes involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between $210$ and $640$ GeV decaying directly to a top quark and a massless LSP is excluded at $95$ % confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at $95$ % confidence level up to a mass of $500$ GeV for an LSP mass in the range of $100$ to $150$ GeV. Stringent exclusion limits are also derived for all other stop decay modes considered, and model-independent upper limits are set on the visible cross-section for processes beyond the Standard Model.
Expected and observed $H_{T,sig}^{miss}$ distribution for tN_med SR, before applying the $H_{T,sig}^{miss}>12$ requirement. The uncertainty includes statistical and all experimental systematic uncertainties. The last bin includes overflows.
Expected and observed large-R jet mass distribution for tN_boost SR, before applying the large-R jet mass$>75$ GeV requirement. The uncertainty includes statistical and all experimental systematic uncertainties. The last bin includes overflows.
Expected and observed b-jet multiplicity distribution for bCc_diag SR, before applying the b-jet multiplicity$=0$ requirement. The uncertainty includes statistical and all experimental systematic uncertainties. The last bin includes overflows.
A search for direct pair production of the supersymmetric partner of the top quark, decaying via a scalar tau to a nearly massless gravitino, has been performed using 20 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=8$ TeV. The data were collected by the ATLAS experiment at the LHC in 2012. Top squark candidates are searched for in events with either two hadronically decaying tau leptons, one hadronically decaying tau and one light lepton, or two light leptons. No significant excess over the Standard Model expectation is found. Exclusion limits at 95% confidence level are set as a function of the top squark and scalar tau masses. Depending on the scalar tau mass, ranging from the 87 GeV LEP limit to the top squark mass, lower limits between 490 GeV and 650 GeV are placed on the top squark mass within the model considered.
Distribution of $m_{\rm T}^{\rm sum}(\tau_{\mathrm{had}},\tau_{\mathrm{had}})$ for the events passing all the hadron-hadron signal region requirements, except that on the variable itself. The SM background process have been normalised using a fit to the data observed in CRs.
Distribution of $m_{{\rm T}2}(\tau_{\mathrm{had}},\tau_{\mathrm{had}})$ for the events passing all the hadron-hadron signal region requirements, except that on the variable itself. The SM background process have been normalised using a fit to the data observed in CRs.
Distribution of $m_{{\rm T}2}(b \ell, b \tau_{\mathrm{had}})$ for events passing all the lepton-hadron LM signal region requirements, except that on the variable itself. The SM background process have been normalised using a fit to the data observed in CRs.
A search is presented for direct top squark pair production using events with at least two leptons including a same-flavour opposite-sign pair with invariant mass consistent with the $Z$ boson mass, jets tagged as originating from $b$-quarks and missing transverse momentum. The analysis is performed with proton-proton collision data at $\sqrt{s}=8$ TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20.3 fb$^{-1}$. No excess beyond the Standard Model expectation is observed. Interpretations of the results are provided in models based on the direct pair production of the heavier top squark state ($\tilde{t}_2$) followed by the decay to the lighter top squark state ($\tilde{t}_1$) via $\tilde{t}_2 \to Z\tilde{t}_1$, and for $\tilde{t}_1$ pair production in natural gauge-mediated supersymmetry breaking scenarios where the neutralino ($\tilde{\chi}^0_1$) is the next-to-lightest supersymmetric particle and decays producing a $Z$ boson and a gravitino ($\tilde{G}$) via the $\tilde{\chi}^0_1 \to Z\tilde{G}$ process.
PT(ll) distribution in SR2A for stop GMSB model (data+/-stat, bkg+/-(stat+syst), signal+/-stat), m(stop1)=500 GeV, m(neutralino1)=400 GeV.
njet_3l (data+/-stat, bkg+/-(stat+syst), signal+/-stat).
Missing ET distribution in SR2A for stop GMSB model (data+/-stat, bkg+/-(stat+syst), signal+/-stat), m(stop1)=500 GeV, m(neutralino1)=400 GeV.
A measurement of jet shapes in top-quark pair events using 1.8 fb$^{-1}$ of $\sqrt{s}$ = 7 TeV pp collision data recorded by the ATLAS detector is presented. Samples of top-quark pair events are selected in both the single-lepton and dilepton final states. The differential and integrated shapes of the jets initiated by bottom-quarks from the top-quark decays are compared with those of the jets originated by light-quarks from the hadronic W-boson decays $W \to q\bar{q}'$ in the single-lepton channel. The light-quark jets are found to have a narrower distribution of the momentum flow inside the jet area than b-quark jets.
Differential jet shape as a function of the radius r for the PT range 30-40 GeV.
Integrated jet shape as a function of the radius r for the PT range 30-40 GeV.
Differential jet shape as a function of the radius r for the PT range 40-50 GeV.
Measurements are presented of differential cross-sections for top quark pair production in pp collisions at sqrt(s) = 7 TeV relative to the total inclusive top quark pair production cross-section. A data sample of 2.05/fb recorded by the ATLAS detector at the Large Hadron Collider is used. Relative differential cross-sections are derived as a function of the invariant mass, the transverse momentum and the rapidity of the top quark pair system. Events are selected in the lepton (electron or muon) + jets channel. The background-subtracted differential distributions are corrected for detector effects, normalized to the total inclusive top quark pair production cross-section and compared to theoretical predictions. The measurement uncertainties range typically between 10% and 20% and are generally dominated by systematic effects. No significant deviations from the Standard Model expectations are observed.
Relative differential cross-section (1/SIG)*D(SIG)/DM(ttbar) measured in the e+jets, mu+jets and the combined lepton+jets channel.
Relative differential cross-section (1/SIG)*D(SIG)/DPT(ttbar) measured in the e+jets, mu+jets and the combined lepton+jets channel.
Relative differential cross-section (1/SIG)*D(SIG)/DYRAP(ttbar) measured in the e+jets, mu+jets and the combined lepton+jets channel.
A search is presented for production of a heavy up-type quark ($t^\prime$) together with its antiparticle, assuming a significant branching ratio for subsequent $t^\prime$ decay into a Standard Model Higgs boson and a top quark, as predicted by vector-like quark models. The search is based on 14.3 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=8$ TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the lepton+jets final state, characterised by an isolated electron or muon with moderately high transverse momentum, significant missing transverse momentum, and at least six jets. The search exploits the high total transverse momenta of all final state objects and the high multiplicity of $b$ jets characteristic of signal events with at least one Higgs boson decaying into $b\bar{b}$, to discriminate against the dominant background from top quark pair production. No significant excess of events above the Standard Model expectation is observed, and upper limits are derived for vector-like quarks of various masses in the two-dimensional plane of $BR(t^\prime \to Wb)$ versus $BR(t^\prime \to Ht)$, where $H$ is the Standard Model Higgs boson, assumed to have a mass of $125$ GeV. Under the branching ratio assumptions corresponding to a weak-isospin doublet (singlet) scenario, a $t^\prime$ quark with mass lower than 790 (640) GeV is excluded at the 95\% confidence level.
The observed and simulated HT distributions in the combined e+jets and mu+jets channels with >=6 jets and 2 b tagged jets.
The observed and simulated HT distributions in the combined e+jets and mu+jets channels with >=6 jets and 3 b tagged jets.
The observed and simulated HT distributions in the combined e+jets and mu+jets channels with >=6 jets and 4 b tagged jets.
The results of a search for pair production of light top squarks are presented, using 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions collected with the ATLAS detector at the Large Hadron Collider. This search targets top squarks with masses similar to, or lighter than, the top quark mass. Final states containing exclusively one or two leptons (e, mu), large missing transverse momentum, light-jets and b-jets are used to reconstruct the top squark pair system. Global mass scale variables are used to separate the signal from a large ttbar background. No excess over the Standard Model expectations is found. The results are interpreted in the framework of the Minimal Supersymmetric Standard Model, assuming the top squark decays exclusively to a chargino and a b-quark. Light top squarks with masses between 123-167 GeV are excluded for neutralino masses around 55 GeV.
Expected 95 PCT exclusion limit in the M(stop), M(neutralino) plane in gaugino universality scenario.
Observed 95 PCT exclusion limit in the M(stop), M(neutralino) plane in gaugino universality scenario.
Expected 95 PCT exclusion limit in the M(chargino), M(neutralino) plane in the scenario where M(stop) = 180 GEV.
The results of a search for the stop, the supersymmetric partner of the top quark, in final states with one isolated electron or muon, jets, and missing transverse momentum are reported. The search uses the 2015 LHC $pp$ collision data at a center-of-mass energy of $\sqrt{s}=13$ TeV recorded by the ATLAS detector and corresponding to an integrated luminosity of 3.2 fb${}^{-1}$. The analysis targets two types of signal models: gluino-mediated pair production of stops with a nearly mass-degenerate stop and neutralino; and direct pair production of stops, decaying to the top quark and the lightest neutralino. The experimental signature in both signal scenarios is similar to that of a top quark pair produced in association with large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits on gluino and stop masses are set at 95% confidence level. The results extend the LHC Run-1 exclusion limit on the gluino mass up to 1460 GeV in the gluino-mediated scenario in the high gluino and low stop mass region, and add an excluded stop mass region from 745 to 780 GeV for the direct stop model with a massless lightest neutralino. The results are also reinterpreted to set exclusion limits in a model of vector-like top quarks.
Comparison of data with estimated backgrounds in the $am_\text{T2}$ distribution with the STCR1 event selection except for the requirement on $am_\text{T2}$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.
Comparison of data with estimated backgrounds in the $b$-tagged jet multiplicity with the STCR1 event selection except for the requirement on the $b$-tagged jet multiplicity. Furthermore, the $\Delta R(b_1,b_2)$ requirement is dropped. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.
Comparison of data with estimated backgrounds in the $\Delta R(b_1,b_2)$ distribution with the STCR1 event selection except for the requirement on $\Delta R(b_1,b_2)$. The predicted backgrounds are scaled with normalization factors. The uncertainty band includes statistical and all experimental systematic uncertainties. The last bin includes overflow.
In the $pp \rightarrow t\bar{t}$ process the angular distributions of top and anti-top quarks are expected to present a subtle difference, which could be enhanced by processes not included in the Standard Model. This Letter presents a measurement of the charge asymmetry in events where the top-quark pair is produced with a large invariant mass. The analysis is performed on 20.3 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} =$ 8 TeV collected by the ATLAS experiment at the LHC, using reconstruction techniques specifically designed for the decay topology of highly boosted top quarks. The charge asymmetry in a fiducial region with large invariant mass of the top-quark pair ($m_{t\bar{t}} > $ 0.75 TeV) and an absolute rapidity difference of the top and anti-top quark candidates within $-$2 $ < |y_t| - |y_{\bar{t}}| <$ 2 is measured to be 4.2 $\pm$ 3.2%, in agreement with the Standard Model prediction at next-to-leading order. A differential measurement in three $t\bar{t}$ mass bins is also presented.
The measured charge asymmetry after the unfolding to parton level in four intervals of the invariant mass of the $t\bar{t}$ system. The phase space is limited to $|(\Delta |y|)|<$ 2. The uncertainties correspond to the sum in quadrature of statistical and systematic uncertainties (for the data) or to the theory uncertainty (for the SM prediction).
Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel, characterized by two high-${p}_{\rm{T}}$ leptons (electrons or muons), are presented using data corresponding to an integrated luminosity of $20.3$ $\textrm{fb}^{-1}$ from $pp$ collisions at a center-of-mass energy of $\sqrt{s} = 8$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A^{\ell\ell}_{\textrm{C}}$ based on the selected leptons and $A^{t\bar{t}}_{\textrm{C}}$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A^{\ell\ell}_{\textrm{C}} = 0.008 \pm 0.006$ and $A^{t\bar{t}}_{\textrm{C}} = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A^{\ell\ell}_{\textrm{C}} = 0.0064 \pm 0.0003 $ and $A^{t\bar{t}}_{\textrm{C}} = 0.0111 \pm 0.0004$.
Unfolded distribution for the inclusive $\Delta|\eta|$ observable in the fiducial volume.
Unfolded distribution for the inclusive $\Delta|y|$ observable in the fiducial volume.
The leptonic inclusive asymmetry in the fiducial volume.
A measurement of the correlations between the polar angles of leptons from the decay of pair-produced $t$ and $\bar{t}$ quarks in the helicity basis is reported, using proton-proton collision data collected by the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 4.6fb$^{-1}$ at a center-of-mass energy of $\sqrt{s}=7$TeV collected during 2011. Candidate events are selected in the dilepton topology with large missing transverse momentum and at least two jets. The angles $\theta_1$ and $\theta_2$ between the charged leptons and the direction of motion of the parent quarks in the $t\bar{t}$ rest frame are sensitive to the spin information, and the distribution of {\mbox{$\cos\theta_1\cdot\cos\theta_2$}} is sensitive to the spin correlation between the $t$ and $\bar{t}$ quarks. The distribution is unfolded to parton level and compared to the next-to-leading order prediction. A good agreement is observed.
The numerical summary of the unfolded $\cos\theta_1\cdot\cos\theta_2$ distribution, with statistical and systematic uncertainties.
The correlation factors for the statistical uncertainties between any two bins of the unfolded distribution.
A search for a massive $W'$ gauge boson decaying to a top quark and a bottom quark is performed with the ATLAS detector in $pp$ collisions at the LHC. The dataset was taken at a centre-of-mass energy of $\sqrt{s} = 8$ TeV and corresponds to 20.3 fb$^{-1}$ of integrated luminosity. This analysis is done in the hadronic decay mode of the top quark, where novel jet substructure techniques are used to identify jets from high-momentum top quarks. This allows for a search for high-mass $W'$ bosons in the range $1.5 - 3.0$ TeV. $b$-tagging is used to identify jets originating from $b$-quarks. The data are consistent with Standard Model background-only expectations, and upper limits at 95% confidence level are set on the $W' \rightarrow tb$ cross section times branching ratio ranging from $0.16$ pb to $0.33$ pb for left-handed $W'$ bosons, and ranging from $0.10$ pb to $0.21$ pb for $W'$ bosons with purely right-handed couplings. Upper limits at 95% confidence level are set on the $W'$-boson coupling to $tb$ as a function of the $W'$ mass using an effective field theory approach, which is independent of details of particular models predicting a $W'$ boson.
m_tb distributions in data in the one b-tag and the two b-tag category, together with background-only fits excluding the region 4-5 TeV which is beyond the range considered for this analysis. Potential WPRIME_L signal shapes in the hadronic top-quark decay channel with gPRIME = gSM are also given for resonance masses of 1.5, 2.0, 2.5 and 3.0 TeV.
Limits at 95% CL on the cross section times branching ratio to TOP BOTTOM for the left-handed and for the right-handed WPRIME model. The expected cross section for WPRIME production with gprime = gSM is also shown.
Observed and expected 95% CL limits on the ratio of coupling gWPRIME_L/gSM (gWPRIME_R/gSM) of the WPRIME_L (WPRIME_R) model as a function of the WPRIME mass.
Various differential cross-sections are measured in top-quark pair ($t\bar{t}$) events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of $4.6$ fb$^{-1}$. The differential cross-sections are presented in terms of kinematic variables, such as momentum, rapidity and invariant mass, of a top-quark proxyreferred to as the pseudo-top-quark as well as the pseudo-top-quark pair system. The dependence of the measurement on theoretical models is minimal. The measurements are performed on $t\bar{t}$ events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a $b$-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the $W$ boson produced by the top-quark decay in events with a single charged lepton. Differential cross-section measurements of the pseudo-top-quark variables are compared with several Monte Carlo models that implement next-to-leading order or leading-order multi-leg matrix-element calculations.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$in the muon channel. The results shown in this table are one of the inputs for the combined results.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $|y(\hat{t}_{\mathrm{h}})|$ in the muon channel. The results shown in this table are one of the inputs for the combined results.
The differential cross-section for pair production of top quarks with high transverse momentum is measured in 20.3 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 8 TeV. The measurement is performed for $t\bar{t}$ events in the lepton+jets channel. The cross-section is reported as a function of the hadronically decaying top quark transverse momentum for values above 300 GeV. The hadronically decaying top quark is reconstructed as an anti-$k_t$ jet with radius parameter $R=1.0$ and identified with jet substructure techniques. The observed yield is corrected for detector effects to obtain a cross-section at particle level in a fiducial region close to the event selection. A parton-level cross-section extrapolated to the full phase space is also reported for top quarks with transverse momentum above 300 GeV. The predictions of a majority of next-to-leading-order and leading-order matrix-element Monte Carlo generators are found to agree with the measured cross-sections.
Fiducial particle-level differential cross-section, with statistical and systematic uncertainties, as a function of the top-jet candidate p_T.
Parton-level differential cross-section, with statistical and systematic uncertainties, as a function of the hadronically decaying top quark p_T.
The individual systematic uncertainties calculated as a percentage of the particle-level differential cross-section $d\sigma_{tt} / d p_{T,ptcl}$ in each bin. Variations on the two sides ("UP" and "DOWN") are separately quoted with their respective signs. Uncertainties smaller than 0.1% are neglected.
The results of a search for pair production of the lighter scalar partners of top quarks in 2.05 fb-1 of pp collisions at sqrt(s) =7 TeV using the ATLAS experiment at the LHC are reported. Scalar top quarks are searched for in events with two same flavour opposite-sign leptons (electrons or muons) with invariant mass consistent with the Z boson mass, large missing transverse momentum and jets in the final state. At least one of the jets is identified as originating from a b-quark. No excess over Standard Model expectations is found. The results are interpreted in the framework of R-parity conserving, gauge mediated Supersymmetry breaking `natural' scenarios, where the neutralino is the next-to-lightest supersymmetric particle. Scalar top quark masses up to 310 GeV are excluded for the lightest neutralino mass between 115 GeV and 230 GeV at 95% confidence level, reaching an exclusion of the scalar top quark mass of 330 GeV for the lightest neutralino mass of 190 GeV. Scalar top quark masses below 240 GeV are excluded for all values of the lightest neutralino mass above the Z boson mass.
The missing ET distribution from the combined EE and MUMU data for SR1. Tabulated are the observed Data rates and the Standard Model predictions as well as the distributions expected for two signal scenarios, both with an STOP mass of 250 GeV, and NEUTRALINO1 masses of 100 GeV and 220 GeV respectively.
The number of b-tagged jets for SR1 for the combined EE and MUMU channels. Tabulated are the observed Data rates and the Standard Model predictions as well as the distributions expected for two signal scenarios, both with an STOP mass of 250 GeV, and NEUTRALINO1 masses of 100 GeV and 220 GeV respectively.
The distrubution of leading jet pT for SR1 for the combined EE and MUMU channels. Tabulated are the observed Data rates and the Standard Model predictions as well as the distributions expected for two signal scenarios, both with an STOP mass of 250 GeV, and NEUTRALINO1 masses of 100 GeV and 220 GeV respectively. The last pT bin includes the number of overflow events for both data abd SM expectation.
A search for direct pair production of supersymmetric top squarks (stop_1) is presented, assuming the stop_1 decays into a top quark and the lightest supersymmetric particle, neutralino_1, and that both top quarks decay to purely hadronic final states. A total of 16 (4) events are observed compared to a predicted Standard Model background of 13.5+3.7-3.6 (4.4+1.7-1.3) events in two signal regions based on int(Ldt) = 4.7 fb^-1 of pp collision data taken at sqrt(s) = 7 TeV with the ATLAS detector at the LHC. An exclusion region in the stop_1 versus neutralino_1 mass plane is evaluated: 370<m(stop_1)<465 GeV is excluded for m(neutralino_1)~0 GeV while m(stop_1)=445 GeV is excluded for m(neutralino_1)<=50 GeV.
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This paper reports inclusive and differential measurements of the $t\bar{t}$ charge asymmetry $A_{\textrm{C}}$ in 20.3 fb$^{-1}$ of $\sqrt{s} = 8$ TeV $pp$ collisions recorded by the ATLAS experiment at the Large Hadron Collider at CERN. Three differential measurements are performed as a function of the invariant mass, transverse momentum and longitudinal boost of the $t\bar{t}$ system. The $t\bar{t}$ pairs are selected in the single-lepton channels ($e$ or $\mu$) with at least four jets, and a likelihood fit is used to reconstruct the $t\bar{t}$ event kinematics. A Bayesian unfolding procedure is performed to infer the asymmetry at parton level from the observed data distribution. The inclusive $t\bar{t}$ charge asymmetry is measured to be $A_{\textrm{C}} = 0.009 \pm 0.005$ (stat.$+$syst.). The inclusive and differential measurements are compatible with the values predicted by the Standard Model.
The inclusive $t\bar{t}$ production charge asymmetry, $A_C$, with statistical and systematic uncertainties combined.
Measured charge asymmetry, $A_C$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ invariant mass, $m_{t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.
Measured charge asymmetry, $A_C$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ velocity along the z-axis, $\beta_{z,t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.
Measurements of normalized differential cross-sections of top quark pair ($t\bar t$) production are presented as a function of the mass, the transverse momentum and the rapidity of the $t\bar t$ system in proton-proton collisions at center-of-mass energies of $\sqrt{s}$ = 7 TeV and 8 TeV. The dataset corresponds to an integrated luminosity of 4.6 fb$^{-1}$ at 7 TeV and 20.2 fb$^{-1}$ at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a $b$-hadron. The measured distributions are corrected for detector effects and selection efficiency to cross-sections at the parton level. The differential cross-sections are compared with different Monte Carlo generators and theoretical calculations of $t\bar t$ production. The results are consistent with the majority of predictions in a wide kinematic range.
Parton-level normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
The inclusive and fiducial $t\bar{t}$ production cross-sections are measured in the lepton+jets channel using 20.2 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of 8 TeV recorded with the ATLAS detector at the LHC. Major systematic uncertainties due to the modelling of the jet energy scale and $b$-tagging efficiency are constrained by separating selected events into three disjoint regions. In order to reduce systematic uncertainties in the most important background, the W+jets process is modelled using Z+jets events in a data-driven approach. The inclusive $t\bar{t}$ cross-section is measured with a precision of 5.7% to be $\sigma_{\text{inc}}(t\bar{t})$ = 248.3 $\pm$ 0.7 (stat.) $\pm$ 13.4 (syst.) $\pm$ 4.7 (lumi.) pb, assuming a top-quark mass of 172.5 GeV. The result is in agreement with the Standard Model prediction. The cross-section is also measured in a phase space close to that of the selected data. The fiducial cross-section is $\sigma_{\text{fid}}(t\bar{t})$ = 48.8 $\pm$ 0.1 (stat.) $\pm$ 2.0 (syst.) $\pm$ 0.9 (lumi.) pb with a precision of 4.5%.
The measured inclusive cross section. The first systematic uncertainty (sys_1) is the combined systematic uncertainty excluding luminosity, the second (sys_2) is the luminosity
The measured fiducial cross section. The first systematic uncertainty (sys_1) is the combined systematic uncertainty excluding luminosity, the second (sys_2) is the luminosity
Measurements of differential cross sections of top quark pair production in association with jets by the ATLAS experiment at the LHC are presented. The measurements are performed as functions of the top quark transverse momentum, the transverse momentum of the top quark-antitop quark system and the out-of-plane transverse momentum using data from $pp$ collisions at $\sqrt{s}=13$ TeV collected by the ATLAS detector at the LHC in 2015 and corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The top quark pair events are selected in the lepton (electron or muon) + jets channel. The measured cross sections, which are compared to several predictions, allow a detailed study of top quark production.
Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration, obtained through the Bootstrap Method.
Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and $p_{T}^{t,had}$ in the 4-jet exclusive configuration, obtained through the Bootstrap Method.
Statistical correlation matrix between |$p_{out}^{t\bar{t}}$| in the 4-jet exclusive configuration and $p_{T}^{t\bar{t}}$ in the 4-jet exclusive configuration, obtained through the Bootstrap Method.
Measurements of differential cross-sections of top-quark pair production in fiducial phase-spaces are presented as a function of top-quark and $t\bar{t}$ system kinematic observables in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$=13 TeV. The data set corresponds to an integrated luminosity of $3.2$ fb${}^{-1}$, recorded in 2015 with the ATLAS detector at the CERN Large Hadron Collider. Events with exactly one electron or muon and at least two jets in the final state are used for the measurement. Two separate selections are applied that each focus on different top-quark momentum regions, referred to as resolved and boosted topologies of the $t\bar{t}$ final state. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations by means of calculated $\chi^2$ and $p$-values.
Covariance matrix of the absolute cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.
Covariance matrix of the absolute cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.
Covariance matrix of the relative cross-section as function of the top quark pT, accounting for the statistical and systematic uncertainties in the resolved topology.
A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm \rightarrow tb$ is presented. The data analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \rightarrow tb H^\pm$, is explored in the mass range from $m_{H^\pm}$ = 200 to 2000 GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching fraction of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm}$ = 200 GeV to 0.070 pb at $m_{H^\pm}$ = 2000 GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.
Expected and observed limits for the production of $H^{+} \to tb$ in association with a top quark and a bottom quark. The bands surrounding the expected limit show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. Theory predictions are shown for three representative values of $\tan\beta$ in the $m_h^{\mathrm{mod-}}$ benchmark scenario. Uncertainties in the predicted $H^+$ cross-sections or branching ratios are not considered.
Expected and observed upper limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the $m_h^{\mathrm{mod-}}$ scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
Expected and observed lower limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the $m_h^{\mathrm{mod-}}$ scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
Measurements of normalized differential cross-sections of top-quark pair production are presented as a function of the top-quark, $t\bar{t}$ system and event-level kinematic observables in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=8$ TeV}. The observables have been chosen to emphasize the $t\bar{t}$ production process and to be sensitive to effects of initial- and final-state radiation, to the different parton distribution functions, and to non-resonant processes and higher-order corrections. The dataset corresponds to an integrated luminosity of 20.3 fb$^{-1}$, recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of the jets tagged as originating from a $b$-quark. The measured spectra are corrected for detector effects and are compared to several Monte Carlo simulations. The results are in fair agreement with the predictions over a wide kinematic range. Nevertheless, most generators predict a harder top-quark transverse momentum distribution at high values than what is observed in the data. Predictions beyond NLO accuracy improve the agreement with data at high top-quark transverse momenta. Using the current settings and parton distribution functions, the rapidity distributions are not well modelled by any generator under consideration. However, the level of agreement is improved when more recent sets of parton distribution functions are used.
Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.
Fiducial phase-space relative differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system invariant mass $m^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.
Fiducial phase-space absolute differential cross-sections after combining the e+jets and $\mu$+jets channels for the $t\bar{t}$ system transverse momentum $p_{T}^{t\bar{t}}$. All uncertainties are quoted as a percentage with respect to the cross-section values in each bin.
A measurement of the top-quark mass ($m_t$) in the $t\bar{t}\rightarrow~\textrm{lepton}+\textrm{jets}$ channel is presented, with an experimental technique which exploits semileptonic decays of $b$-hadrons produced in the top-quark decay chain. The distribution of the invariant mass $m_{\ell\mu}$ of the lepton, $\ell$ (with $\ell=e,\mu$), from the $W$-boson decay and the muon, $\mu$, originating from the $b$-hadron decay is reconstructed, and a binned-template profile likelihood fit is performed to extract $m_t$. The measurement is based on data corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of $\sqrt{s} = 13~\textrm{TeV}$$pp$ collisions provided by the Large Hadron Collider and recorded by the ATLAS detector. The measured value of the top-quark mass is $m_{t} = 174.41\pm0.39~(\textrm{stat.})\pm0.66~(\textrm{syst.})\pm0.25~(\textrm{recoil})~\textrm{GeV}$, where the third uncertainty arises from changing the PYTHIA8 parton shower gluon-recoil scheme, used in top-quark decays, to a recently developed setup.
Top mass measurement result.
List of all the individual sources of systematic uncertainty considered in the analysis. The individual sources, each corresponding to an independent nuisance parameter in the fit, are grouped into categories, as indicated in the first column. The second column shows the impact of each of the individual sources on the measurement, obtained as the shift on the top mass induced by a positive shift of the each of the nuisance parameters by its post-fit uncertainty. Sources for which no impact is indicated are neglected in the fit procedure as their impact on the total prediction is negligible in any of the bins. The last column shows the statistical uncertainty in each of the reported numbers as estimated with the bootstrap method.
Ranking, from top to bottom, of the main systematic uncertainties (excluding recoil) showing the pulls and the impact of the systematic uncertainties on the top mass, from the combined opposite sign (OS) and same sign (SS) binned-template profile likelihood fit to data. The OS or SS refers to the charge signs of the primary lepton and the soft muon. The gamma parameters are NPs used to describe the effect of the limited statistics of the sample.
A measurement of jet substructure variables is presented using data collected in 2016 by the ATLAS experiment at the LHC with proton-proton collisions at $\sqrt{s}=13$ TeV. Large-radius jets groomed with the trimming and soft-drop algorithms are studied. Dedicated event selections are used to study jets produced by light quarks or gluons, and hadronically decaying top quarks and $W$ bosons. The variables measured are sensitive to pronged substructure, and therefore are typically used for tagging jets from boosted massive particles. These include the energy correlation functions and the $N$-subjettiness variables. The number of subjets and the Les Houches angularity are also considered. The distributions of the substructure variables, corrected for detector effects, are compared to the predictions of various Monte Carlo event generators. They are also compared between the large-radius jets originating from light quarks or gluons, and hadronically decaying top quarks and $W$ bosons.
Figure 3a, Normalised differential Nsubjets distribution for soft-drop groomed jets, Dijet selection.
Figure 4a, Normalised differential LHA distribution for soft-drop groomed jets, Dijet selection
Figure 5a, Normalised differential C2 distribution for soft-drop groomed jets, Dijet selection
This article presents measurements of the $t$-channel single top-quark ($t$) and top-antiquark ($\bar{t}$) total production cross sections $\sigma(tq)$ and $\sigma(\bar{t}q)$, their ratio $R_{t}=\sigma(tq)/\sigma(\bar{t}q)$, and a measurement of the inclusive production cross section $\sigma(tq + \bar{t}q)$ in proton--proton collisions at $\sqrt{s} = 7$ TeV at the LHC. Differential cross sections for the $tq$ and $\bar{t}q$ processes are measured as a function of the transverse momentum and the absolute value of the rapidity of $t$ and $\bar{t}$, respectively. The analyzed data set was recorded with the ATLAS detector and corresponds to an integrated luminosity of 4.59 fb$^{-1}$. Selected events contain one charged lepton, large missing transverse momentum, and two or three jets. The cross sections are measured by performing a binned maximum-likelihood fit to the output distributions of neural networks. The resulting measurements are $\sigma(tq)= 46\pm 6\; \mathrm{pb}$, $\sigma(\bar{t}q)= 23 \pm 4\; \mathrm{pb}$, $R_{t}=2.04\pm 0.18$, and $\sigma(tq + \bar{t}q)= 68 \pm 8\; \mathrm{pb}$, consistent with the Standard Model expectation. The uncertainty on the measured cross sections is dominated by systematic uncertainties, while the uncertainty on $R_{t}$ is mainly statistical. Using the ratio of $\sigma(tq + \bar{t}q)$ to its theoretical prediction, and assuming that the top-quark-related CKM matrix elements obey the relation $|V_{tb}|\gg |V_{ts}|, |V_{td}|$, we determine $|V_{tb}|=1.02 \pm 0.07$.
Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of PT(TOP).
Predicted and observed events yields for the 2-jet and 3-jet channels considered in this measurement. The multijet background is estimated using data-driven techniques (see Sec. VB); an uncertainty of $50\%$ is applied. All the other expectations are derived using theoretical cross sections and their uncertainties (see Secs. VA and VC in the paper).
Differential t-channel top-quark production cross sections and normalized differential t-channel top-quark production cross sections as functions of PT(TOPBAR).
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/>
Relative differential cross-section as a function of $p_{T}^{t,had}$ at particle level in the resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t,had}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
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/>
Relative differential cross-section as a function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.
Measurements of $K_S^0$ and $\Lambda^0$ production in $t\bar{t}$ final states have been performed. They are based on a data sample with integrated luminosity of 4.6 $\mathrm{fb}^{-1}$ from proton-proton collisions at a centre-of-mass energy of 7 TeV, collected in 2011 with the ATLAS detector at the Large Hadron Collider. Neutral strange particles are separated into three classes, depending on whether they are contained in a jet, with or without a $b$-tag, or not associated with a selected jet. The aim is to look for differences in their main kinematic distributions. A comparison of data with several Monte Carlo simulations using different hadronisation and fragmentation schemes, colour reconnection models and different tunes for the underlying event has been made. The production of neutral strange particles in $t\bar{t}$ dileptonic events is found to be well described by current Monte Carlo models for $K_S^0$ and $\Lambda^0$ production within jets, but not for those produced outside jets.
The transverse momentum ($p_{T}$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking inefficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.
The energy fraction ($x_{K}$) distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.
The energy distribution for $K^{0}_{S}$ production inside $b$-jets for unfolded data to particle level, normalised to the total number of top pair dileptonic events and scaled to the bin width. The systematic uncertainties are, in order, due to; the MC modelling, the tracking ineficiencies, the jet energy scale (JES), the jet energy resolution (JER), out-of-fiducial events and the unfolding non-closure.
A measurement of single top-quark production in the s-channel is performed in proton$-$proton collisions at a centre-of-mass energy of 13 TeV with the ATLAS detector at the CERN Large Hadron Collider. The dataset corresponds to an integrated luminosity of 139 fb$^{-1}$. The analysis is performed on events with an electron or muon, missing transverse momentum and exactly two $b$-tagged jets in the final state. A discriminant based on matrix element calculations is used to separate single-top-quark s-channel events from the main background contributions, which are top-quark pair production and $W$-boson production in association with jets. The observed (expected) signal significance over the background-only hypothesis is 3.3 (3.9) standard deviations, and the measured cross-section is $\sigma=8.2^{+3.5}_{-2.9}$ pb, consistent with the Standard Model prediction of $\sigma^{\mathrm{SM}}=10.32^{+0.40}_{-0.36}$ pb.
Result of the s-channel single-top cross-section measurement, in pb. The statistical and systematic uncertainties are given, as well as the total uncertainty. The normalisation factors for the $t\bar{t}$ and $W$+jets backgrounds are also shown, with their total uncertainties.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the signal region, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
Distribution of ${E}_{T}^{miss}$ after the fit of the multijet backgrounds, in the electron channel, in the $W$+jets VR, without applying the cut on ${E}_{T}^{miss}$. Simulated events are normalised to the expected number of events given the integrated luminosity, after applying the normalisation factors obtained in the multijet fit. The last bin includes the overflow. The uncertainty band indicates the simulation's statistical uncertainty, the normalisation uncertainties for different processes ($40$ % for $W$+jets production, $30$ % for multijet background and $6$ % for top-quark processes) and the multijet background shape uncertainty in each bin, summed in quadrature. The lower panel of the figure shows the ratio of the data to the prediction.
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