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No description provided.
No description provided.
No description provided.
Results on K 0 and Λ production in p↑p interactions at 6 GeV are presented. The data are from an exposure of the Argonne 12 ft bubble chamber to a 60% transversely polarized proton beam. Results include data on Λ and K 0 inclusive production, and on the reactions p↑p → p Λ K + (p Σ 0 K + ). The beam asymmetry parameter for p ↑ p → K 0 ( K 0 ) + X is determined to be (−0.52 ± 0.12).
No description provided.
We have studied inclusive KS0, Λ, and Λ¯ production in π+d interactions at 24 GeV/c. The observed cross sections are 2.5±0.13 mb for KS0, 1.62±0.09 mb for Λ, and 0.12±0.02 mb for Λ¯. Longitudinal- and transverse-momentum distributions of the produced particles are presented. The average charged multiplicities of the system associated with a KS0 or with a Λ are presented and discussed. A nonzero average Λ polarization (-0.10±0.03) is observed. The x distribution of the backward (forward) KS0 and Λ produced in the reaction are in agreement with the x distribution of valence quarks in nucleons in nuclear target (pion beam), as predicted by the quark-recombination model of particle production applied to nuclear targets.
Axis error includes +- 0.0/0.0 contribution (?////THE QUOTED IN THE TABLES ERROR INCLUDE ESTIMATES OF UNCERTAINTY IN EACH OF THE CORRECTIONS MADE IN ADDITION TO THE STATISTICAL ERRORCORRECTIONS HAVE BEEN MADE FOR DETECTION, MEASURING, AND FITTING LOSSES AS WELL AS FOR NEUTRAL DECAY MODES OF THE STRANGE PARTICLESNO CORRECTION WAS MADE FOR CONTAMINATION FROM KL'S NOR FOR UNAVOIDABLE INCLUSION OF SIGMA0 EVENTS).
Axis error includes +- 0.0/0.0 contribution (?////THE QUOTED IN THE TABLES ERROR INCLUDE ESTIMATES OF UNCERTAINTY IN EACH OF THE CORRECTIONS MADE IN ADDITION TO THE STATISTICAL ERRORCORRECTIONS HAVE BEEN MADE FOR DETECTION, MEASURING, AND FITTING LOSSES AS WELL AS FOR NEUTRAL DECAY MODES OF THE STRANGE PARTICLESNO CORRECTION WAS MADE FOR CONTAMINATION FROM KL'S NOR FOR UNAVOIDABLE INCLUSION OF SIGMA0 EVENTS).
Axis error includes +- 0.0/0.0 contribution (?////THE QUOTED IN THE TABLES ERROR INCLUDE ESTIMATES OF UNCERTAINTY IN EACH OF THE CORRECTIONS MADE IN ADDITION TO THE STATISTICAL ERRORCORRECTIONS HAVE BEEN MADE FOR DETECTION, MEASURING, AND FITTING LOSSES AS WELL AS FOR NEUTRAL DECAY MODES OF THE STRANGE PARTICLESNO CORRECTION WAS MADE FOR CONTAMINATION FROM KL'S NOR FOR UNAVOIDABLE INCLUSION OF SIGMA0 EVENTS).
A search is performed for resonant and non-resonant Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state. The data set used corresponds to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No significant excess relative to the Standard Model expectation is observed. The observed limit on the non-resonant Higgs boson pair cross-section is 0.73 pb at 95% confidence level. This observed limit is equivalent to 22 times the predicted Standard Model cross-section. The Higgs boson self-coupling ($\kappa_\lambda = \lambda_{HHH} / \lambda_{HHH}^{\rm SM}$) is constrained at 95% confidence level to $-8.2 < \kappa_\lambda < 13.2$. For resonant Higgs boson pair production through X $\rightarrow$ HH $\rightarrow$ $\gamma\gamma b\bar{b}$, the limit is presented, using the narrow-width approximation, as a function of $m_X$ in the range 260 GeV $< m_X <$ 1000 GeV. The observed limits range from 1.1 pb to 0.12 pb over this mass range.
The 95% CL observed and expected limits on the Higgs boson pair cross-section in picobarn and as a multiple of the SM production cross-section. The expected 1 sigma CLs bands are also indicated.
Expected and observed upper limits at the 95% CL on the cross-section of gluon-fusion initiated Higgs boson pair production as a function of $\kappa_{\lambda}$.
Expected and observed upper limits at the 95% CL on the cross-section of gluon-fusion initiated resonant production of a Higgs boson pair as a function of the mass of the resonance, $m_X$.
A search for a heavy charged-boson resonance decaying into a charged lepton (electron or muon) and a neutrino is reported. A data sample of 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s} = 13$ TeV collected with the ATLAS detector at the LHC during 2015-2018 is used in the search. The observed transverse mass distribution computed from the lepton and missing transverse momenta is consistent with the distribution expected from the Standard Model, and upper limits on the cross section for $pp \to W^\prime \to \ell\nu$ are extracted ($\ell = e$ or $\mu$). These vary between 1.3 pb and 0.05 fb depending on the resonance mass in the range between 0.15 and 7.0 TeV at 95% confidence level for the electron and muon channels combined. Gauge bosons with a mass below 6.0 TeV and 5.1 TeV are excluded in the electron and muon channels, respectively, in a model with a resonance that has couplings to fermions identical to those of the Standard Model $W$ boson. Cross-section limits are also provided for resonances with several fixed $\Gamma / m$ values in the range between 1% and 15%. Model-independent limits are derived in single-bin signal regions defined by a varying minimum transverse mass threshold. The resulting visible cross-section upper limits range between 4.6 (15) pb and 22 (22) ab as the threshold increases from 130 (110) GeV to 5.1 (5.1) TeV in the electron (muon) channel.
Upper limits at the 95% CL on the cross section for SSM $W^\prime$ production and decay to the electron+neutrino channel as a function of the $W^\prime$ pole mass.
Upper limits at the 95% CL on the cross section for SSM $W^\prime$ production and decay to the muon+neutrino channel as a function of the $W^\prime$ pole mass.
Combined (electron and muon channels) upper limits at the 95% CL on the cross section for SSM $W^\prime$ production and decay to a single lepton generation as a function of the $W^\prime$ pole mass.
A search for flavour-changing neutral current (FCNC) events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81 fb$^{-1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95% CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t\rightarrow \gamma u$ of $2.8\times 10^{-5}$ ($6.1\times 10^{-5}$). In addition, they are interpreted as 95% CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t\rightarrow \gamma c$ of $22\times 10^{-5}$ ($18\times 10^{-5}$).
Post-fit distributions of a background-only fit to the signal region (SR) and the control regions (CRs) of the NN output in the SR. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
Observed (expected) 95 % CL limits on the effective coupling strengths for different vertices and couplings, the production cross section, and the branching ratio. For the former, the energy scale is assumed to be $\Lambda$ = 1 TeV.
Post-fit distributions of a background-only fit to the SR and the CRs of the NN output in the SR for the $tu\gamma$ right-handed coupling. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
A search for new phenomena in events with two same-charge leptons or three leptons and jets identified as originating from $b$-quarks in a data sample of 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}= 13$ TeV recorded by the ATLAS detector at the Large Hadron Collider is reported. No significant excess is found and limits are set on vector-like quark, four-top-quark, and same-sign top-quark pair production. The observed (expected) 95% CL mass limits for a vector-like $T$- and $B$-quark singlet are $m_T > 0.98$ $(0.99)$ TeV and $m_B > 1.00$ $(1.01)$ TeV respectively. Limits on the production of the vector-like $T_{5/3}$-quark are also derived considering both pair and single production; in the former case the lower limit on the mass of the $T_{5/3}$-quark is (expected to be) 1.19 (1.21) TeV. The Standard Model four-top-quark production cross-section upper limit is (expected to be) 69 (29) fb. Constraints are also set on exotic four-top-quark production models. Finally, limits are set on same-sign top-quark pair production. The upper limit on $uu \to tt$ production is (expected to be) 89 (59) fb for a mediator mass of 1 TeV, and a dark-matter interpretation is also derived, excluding a mediator of 3 TeV with a dark-sector coupling of 1.0 and a coupling to ordinary matter above 0.31.
Expected and observed limits on vector-like B-quark pair production as a function of mass, assuming the branching ratios expected in the singlet model.
Expected and observed limits on vector-like B-quark pair production as a function of mass, assuming the branching ratios expected in the singlet model.
Expected and observed limits on vector-like T-quark pair production as a function of mass, assuming the branching ratios expected in the singlet model.
Statistical combinations of searches for charginos and neutralinos using various decay channels are performed using $139\,$fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=13\,$TeV with the ATLAS detector at the Large Hadron Collider. Searches targeting pure-wino chargino pair production, pure-wino chargino-neutralino production, or higgsino production decaying via Standard Model $W$, $Z$, or $h$ bosons are combined to extend the mass reach to the produced SUSY particles by 30-100 GeV. The depth of the sensitivity of the original searches is also improved by the combinations, lowering the 95% CL cross-section upper limits by 15%-40%.
Expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.
$+1\sigma$ expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.
$-1\sigma$ expected 95% CL exclusion limits on the simplified models of chargino-pair production decaying via W bosons.
A search for the electroweak production of charginos and sleptons decaying into final states with two electrons or muons is presented. The analysis is based on 139 fb$^{-1}$ of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at $\sqrt{s}=13$ TeV. Three $R$-parity-conserving scenarios where the lightest neutralino is the lightest supersymmetric particle are considered: the production of chargino pairs with decays via either $W$ bosons or sleptons, and the direct production of slepton pairs. The analysis is optimised for the first of these scenarios, but the results are also interpreted in the others. No significant deviations from the Standard Model expectations are observed and limits at 95 % confidence level are set on the masses of relevant supersymmetric particles in each of the scenarios. For a massless lightest neutralino, masses up to 420 GeV are excluded for the production of the lightest-chargino pairs assuming $W$-boson-mediated decays and up to 1 TeV for slepton-mediated decays, whereas for slepton-pair production masses up to 700 GeV are excluded assuming three generations of mass-degenerate sleptons.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Background Fit results:</b> <ul> <li><a href="89413?version=1&table=Backgroundfit1">CRs</a> <li><a href="89413?version=1&table=Backgroundfit2">VRs</a> <li><a href="89413?version=1&table=Backgroundfit5">inclusive DF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit6">inclusive DF-1J SRs</a> <li><a href="89413?version=1&table=Backgroundfit3">inclusive SF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit4">inclusive SF-1J SRs</a> </ul> <b>Kinematic distributions in VRs:</b> <ul> <li><a href="89413?version=1&table=VRkinematics1">$m_{T2}$ in VR-top-low</a> <li><a href="89413?version=1&table=VRkinematics2">$m_{T2}$ in VR-top-high</a> <li><a href="89413?version=1&table=VRkinematics3">$E_T^{miss}$ in VR-WW-0J</a> <li><a href="89413?version=1&table=VRkinematics4">$E_T^{miss}$ in VR-WW-1J</a> <li><a href="89413?version=1&table=VRkinematics5">$E_T^{miss}$ sig in VR-VZ</a> <li><a href="89413?version=1&table=VRkinematics6">$E_T^{miss}$ sig in VR-top-WW</a> </ul> <b>Kinematic distributions in SRs:</b> <ul> <li><a href="89413?version=1&table=SRkinematics1">$m_{T2}$ in SR-SF-0J</a> <li><a href="89413?version=1&table=SRkinematics2">$m_{T2}$ in SR-SF-1J</a> <li><a href="89413?version=1&table=SRkinematics3">$m_{T2}$ in SR-DF-0J</a> <li><a href="89413?version=1&table=SRkinematics4">$m_{T2}$ in SR-DF-1J</a> </ul> <b>Systematic uncertaities:</b> <ul> <li><a href="89413?version=1&table=Systematic uncertainties">dominant systematic uncertainties in the inclusive SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=1&table=Exclusioncontour(obs)1">expected exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)1">observed exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)2">expected exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)2">observed exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)3">expected exclusion contour direct slepton-pair production grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)3">observed exclusion contour direct slepton-pair production grid</a> </ul> <br/><br/><b>AUXILIARY MATERIAL</b><br/> <b>Background Fit in binned SRs:</b> <ul> <li><a href="89413?version=1&table=Backgroundfit7">binned DF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit8">binned DF-1J SRs</a> <li><a href="89413?version=1&table=Backgroundfit9">binned SF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit10">binned SF-1J SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=1&table=Exclusioncontour(obs)4">expected exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)4">observed exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)5">expected exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)5">observed exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)6">expected exclusion contour selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)6">observed exclusion contour selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)7">expected exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)7">observed exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)8">expected exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)8">observed exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)9">expected exclusion contour smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)9">observed exclusion contour smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)10">expected exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)10">observed exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)11">expected exclusion contour right-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)11">observed exclusion contour right-handed smuon-pair production</a> </ul> <b>Cross section upper limits:</b> <ul> <li><a href="89413?version=1&table=xsecupperlimits1">upper limits on signal cross section for direct chargino-pair production via W decay</a> <li><a href="89413?version=1&table=xsecupperlimits2">upper limits on signal cross section for direct chargino-pair production via slepton decay</a> <li><a href="89413?version=1&table=xsecupperlimits3">upper limits on signal cross section for direct slepton-pair production</a> </ul> <b>Acceptances and Efficiencies for direct chargino-pair production via W decay grid </b> <ul> <li> <b>Acceptance</b> <br/> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,inf)forC1C1WWgrid">SR-DF-0J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[160,inf)forC1C1WWgrid">SR-DF-0J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,120)forC1C1WWgrid">SR-DF-0J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[120,160)forC1C1WWgrid">SR-DF-0J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,105)forC1C1WWgrid">SR-DF-0J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[105,110)forC1C1WWgrid">SR-DF-0J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[110,120)forC1C1WWgrid">SR-DF-0J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[120,140)forC1C1WWgrid">SR-DF-0J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[140,160)forC1C1WWgrid">SR-DF-0J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[160,180)forC1C1WWgrid">SR-DF-0J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[180,220)forC1C1WWgrid">SR-DF-0J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[220,260)forC1C1WWgrid">SR-DF-0J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[260,inf)forC1C1WWgrid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,inf)forC1C1WWgrid">SR-DF-1J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[160,inf)forC1C1WWgrid">SR-DF-1J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,120)forC1C1WWgrid">SR-DF-1J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[120,160)forC1C1WWgrid">SR-DF-1J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,105)forC1C1WWgrid">SR-DF-1J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[105,110)forC1C1WWgrid">SR-DF-1J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[110,120)forC1C1WWgrid">SR-DF-1J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[120,140)forC1C1WWgrid">SR-DF-1J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[140,160)forC1C1WWgrid">SR-DF-1J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[160,180)forC1C1WWgrid">SR-DF-1J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[180,220)forC1C1WWgrid">SR-DF-1J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[220,260)forC1C1WWgrid">SR-DF-1J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[260,inf)forC1C1WWgrid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,inf)forC1C1WWgrid">SR-SF-0J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[160,inf)forC1C1WWgrid">SR-SF-0J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,120)forC1C1WWgrid">SR-SF-0J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[120,160)forC1C1WWgrid">SR-SF-0J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,105)forC1C1WWgrid">SR-SF-0J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[105,110)forC1C1WWgrid">SR-SF-0J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[110,120)forC1C1WWgrid">SR-SF-0J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[120,140)forC1C1WWgrid">SR-SF-0J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[140,160)forC1C1WWgrid">SR-SF-0J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[160,180)forC1C1WWgrid">SR-SF-0J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[180,220)forC1C1WWgrid">SR-SF-0J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[220,260)forC1C1WWgrid">SR-SF-0J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[260,inf)forC1C1WWgrid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,inf)forC1C1WWgrid">SR-SF-1J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[160,inf)forC1C1WWgrid">SR-SF-1J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,120)forC1C1WWgrid">SR-SF-1J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[120,160)forC1C1WWgrid">SR-SF-1J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,105)forC1C1WWgrid">SR-SF-1J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[105,110)forC1C1WWgrid">SR-SF-1J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[110,120)forC1C1WWgrid">SR-SF-1J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[120,140)forC1C1WWgrid">SR-SF-1J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[140,160)forC1C1WWgrid">SR-SF-1J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[160,180)forC1C1WWgrid">SR-SF-1J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[180,220)forC1C1WWgrid">SR-SF-1J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[220,260)forC1C1WWgrid">SR-SF-1J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[260,inf)forC1C1WWgrid">SR-SF-1J-[260,inf) </a><br/> <li> <b>Efficiency</b> <br/> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,inf)forC1C1WWgrid">SR-DF-0J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[160,inf)forC1C1WWgrid">SR-DF-0J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,120)forC1C1WWgrid">SR-DF-0J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[120,160)forC1C1WWgrid">SR-DF-0J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,105)forC1C1WWgrid">SR-DF-0J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[105,110)forC1C1WWgrid">SR-DF-0J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[110,120)forC1C1WWgrid">SR-DF-0J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[120,140)forC1C1WWgrid">SR-DF-0J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[140,160)forC1C1WWgrid">SR-DF-0J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[160,180)forC1C1WWgrid">SR-DF-0J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[180,220)forC1C1WWgrid">SR-DF-0J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[220,260)forC1C1WWgrid">SR-DF-0J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[260,inf)forC1C1WWgrid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,inf)forC1C1WWgrid">SR-DF-1J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[160,inf)forC1C1WWgrid">SR-DF-1J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,120)forC1C1WWgrid">SR-DF-1J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[120,160)forC1C1WWgrid">SR-DF-1J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,105)forC1C1WWgrid">SR-DF-1J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[105,110)forC1C1WWgrid">SR-DF-1J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[110,120)forC1C1WWgrid">SR-DF-1J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[120,140)forC1C1WWgrid">SR-DF-1J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[140,160)forC1C1WWgrid">SR-DF-1J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[160,180)forC1C1WWgrid">SR-DF-1J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[180,220)forC1C1WWgrid">SR-DF-1J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[220,260)forC1C1WWgrid">SR-DF-1J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[260,inf)forC1C1WWgrid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,inf)forC1C1WWgrid">SR-SF-0J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[160,inf)forC1C1WWgrid">SR-SF-0J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,120)forC1C1WWgrid">SR-SF-0J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[120,160)forC1C1WWgrid">SR-SF-0J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,105)forC1C1WWgrid">SR-SF-0J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[105,110)forC1C1WWgrid">SR-SF-0J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[110,120)forC1C1WWgrid">SR-SF-0J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[120,140)forC1C1WWgrid">SR-SF-0J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[140,160)forC1C1WWgrid">SR-SF-0J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[160,180)forC1C1WWgrid">SR-SF-0J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[180,220)forC1C1WWgrid">SR-SF-0J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[220,260)forC1C1WWgrid">SR-SF-0J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[260,inf)forC1C1WWgrid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,inf)forC1C1WWgrid">SR-SF-1J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[160,inf)forC1C1WWgrid">SR-SF-1J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,120)forC1C1WWgrid">SR-SF-1J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[120,160)forC1C1WWgrid">SR-SF-1J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,105)forC1C1WWgrid">SR-SF-1J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[105,110)forC1C1WWgrid">SR-SF-1J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[110,120)forC1C1WWgrid">SR-SF-1J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[120,140)forC1C1WWgrid">SR-SF-1J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[140,160)forC1C1WWgrid">SR-SF-1J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[160,180)forC1C1WWgrid">SR-SF-1J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[180,220)forC1C1WWgrid">SR-SF-1J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[220,260)forC1C1WWgrid">SR-SF-1J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[260,inf)forC1C1WWgrid">SR-SF-1J-[260,inf) </a><br/> </ul> <b>Cutflow:</b> <ul> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct chargino-pair production via W decay $m(\tilde{\chi}^{\pm}_1,\tilde{\chi}^{0}_1)=(300,50) GeV$</a> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct chargino-pair production via slepton decay $m(\tilde{\chi}^{\pm}_1,\tilde{l},\tilde{\chi}^{0}_1)=(600,300,1) GeV$</a> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct slepton-pair production $m(\tilde{l},\tilde{\chi}^{0}_1)=(400,200) GeV$</a> </ul> <b>Truth Code snippets</b> are available under "Resources" (purple button on the left)
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Background Fit results:</b> <ul> <li><a href="89413?version=1&table=Backgroundfit1">CRs</a> <li><a href="89413?version=1&table=Backgroundfit2">VRs</a> <li><a href="89413?version=1&table=Backgroundfit5">inclusive DF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit6">inclusive DF-1J SRs</a> <li><a href="89413?version=1&table=Backgroundfit3">inclusive SF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit4">inclusive SF-1J SRs</a> </ul> <b>Kinematic distributions in VRs:</b> <ul> <li><a href="89413?version=1&table=VRkinematics1">$m_{T2}$ in VR-top-low</a> <li><a href="89413?version=1&table=VRkinematics2">$m_{T2}$ in VR-top-high</a> <li><a href="89413?version=1&table=VRkinematics3">$E_T^{miss}$ in VR-WW-0J</a> <li><a href="89413?version=1&table=VRkinematics4">$E_T^{miss}$ in VR-WW-1J</a> <li><a href="89413?version=1&table=VRkinematics5">$E_T^{miss}$ sig in VR-VZ</a> <li><a href="89413?version=1&table=VRkinematics6">$E_T^{miss}$ sig in VR-top-WW</a> </ul> <b>Kinematic distributions in SRs:</b> <ul> <li><a href="89413?version=1&table=SRkinematics1">$m_{T2}$ in SR-SF-0J</a> <li><a href="89413?version=1&table=SRkinematics2">$m_{T2}$ in SR-SF-1J</a> <li><a href="89413?version=1&table=SRkinematics3">$m_{T2}$ in SR-DF-0J</a> <li><a href="89413?version=1&table=SRkinematics4">$m_{T2}$ in SR-DF-1J</a> </ul> <b>Systematic uncertaities:</b> <ul> <li><a href="89413?version=1&table=Systematic uncertainties">dominant systematic uncertainties in the inclusive SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=1&table=Exclusioncontour(obs)1">expected exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)1">observed exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)2">expected exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)2">observed exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)3">expected exclusion contour direct slepton-pair production grid</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)3">observed exclusion contour direct slepton-pair production grid</a> </ul> <br/><br/><b>AUXILIARY MATERIAL</b><br/> <b>Background Fit in binned SRs:</b> <ul> <li><a href="89413?version=1&table=Backgroundfit7">binned DF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit8">binned DF-1J SRs</a> <li><a href="89413?version=1&table=Backgroundfit9">binned SF-0J SRs</a> <li><a href="89413?version=1&table=Backgroundfit10">binned SF-1J SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=1&table=Exclusioncontour(obs)4">expected exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)4">observed exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)5">expected exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)5">observed exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)6">expected exclusion contour selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)6">observed exclusion contour selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)7">expected exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)7">observed exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)8">expected exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)8">observed exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)9">expected exclusion contour smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)9">observed exclusion contour smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)10">expected exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)10">observed exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(obs)11">expected exclusion contour right-handed smuon-pair production</a> <li><a href="89413?version=1&table=Exclusioncontour(exp)11">observed exclusion contour right-handed smuon-pair production</a> </ul> <b>Cross section upper limits:</b> <ul> <li><a href="89413?version=1&table=xsecupperlimits1">upper limits on signal cross section for direct chargino-pair production via W decay</a> <li><a href="89413?version=1&table=xsecupperlimits2">upper limits on signal cross section for direct chargino-pair production via slepton decay</a> <li><a href="89413?version=1&table=xsecupperlimits3">upper limits on signal cross section for direct slepton-pair production</a> </ul> <b>Acceptances and Efficiencies for direct chargino-pair production via W decay grid </b> <ul> <li> <b>Acceptance</b> <br/> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,inf)forC1C1WWgrid">SR-DF-0J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[160,inf)forC1C1WWgrid">SR-DF-0J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,120)forC1C1WWgrid">SR-DF-0J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[120,160)forC1C1WWgrid">SR-DF-0J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[100,105)forC1C1WWgrid">SR-DF-0J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[105,110)forC1C1WWgrid">SR-DF-0J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[110,120)forC1C1WWgrid">SR-DF-0J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[120,140)forC1C1WWgrid">SR-DF-0J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[140,160)forC1C1WWgrid">SR-DF-0J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[160,180)forC1C1WWgrid">SR-DF-0J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[180,220)forC1C1WWgrid">SR-DF-0J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[220,260)forC1C1WWgrid">SR-DF-0J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-DF-0J-[260,inf)forC1C1WWgrid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,inf)forC1C1WWgrid">SR-DF-1J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[160,inf)forC1C1WWgrid">SR-DF-1J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,120)forC1C1WWgrid">SR-DF-1J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[120,160)forC1C1WWgrid">SR-DF-1J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[100,105)forC1C1WWgrid">SR-DF-1J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[105,110)forC1C1WWgrid">SR-DF-1J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[110,120)forC1C1WWgrid">SR-DF-1J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[120,140)forC1C1WWgrid">SR-DF-1J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[140,160)forC1C1WWgrid">SR-DF-1J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[160,180)forC1C1WWgrid">SR-DF-1J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[180,220)forC1C1WWgrid">SR-DF-1J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[220,260)forC1C1WWgrid">SR-DF-1J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-DF-1J-[260,inf)forC1C1WWgrid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,inf)forC1C1WWgrid">SR-SF-0J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[160,inf)forC1C1WWgrid">SR-SF-0J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,120)forC1C1WWgrid">SR-SF-0J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[120,160)forC1C1WWgrid">SR-SF-0J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[100,105)forC1C1WWgrid">SR-SF-0J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[105,110)forC1C1WWgrid">SR-SF-0J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[110,120)forC1C1WWgrid">SR-SF-0J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[120,140)forC1C1WWgrid">SR-SF-0J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[140,160)forC1C1WWgrid">SR-SF-0J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[160,180)forC1C1WWgrid">SR-SF-0J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[180,220)forC1C1WWgrid">SR-SF-0J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[220,260)forC1C1WWgrid">SR-SF-0J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-SF-0J-[260,inf)forC1C1WWgrid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,inf)forC1C1WWgrid">SR-SF-1J-[100,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[160,inf)forC1C1WWgrid">SR-SF-1J-[160,inf) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,120)forC1C1WWgrid">SR-SF-1J-[100,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[120,160)forC1C1WWgrid">SR-SF-1J-[120,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[100,105)forC1C1WWgrid">SR-SF-1J-[100,105) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[105,110)forC1C1WWgrid">SR-SF-1J-[105,110) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[110,120)forC1C1WWgrid">SR-SF-1J-[110,120) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[120,140)forC1C1WWgrid">SR-SF-1J-[120,140) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[140,160)forC1C1WWgrid">SR-SF-1J-[140,160) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[160,180)forC1C1WWgrid">SR-SF-1J-[160,180) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[180,220)forC1C1WWgrid">SR-SF-1J-[180,220) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[220,260)forC1C1WWgrid">SR-SF-1J-[220,260) </a> <a href="89413?version=1&table=AcceptanceSR-SF-1J-[260,inf)forC1C1WWgrid">SR-SF-1J-[260,inf) </a><br/> <li> <b>Efficiency</b> <br/> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,inf)forC1C1WWgrid">SR-DF-0J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[160,inf)forC1C1WWgrid">SR-DF-0J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,120)forC1C1WWgrid">SR-DF-0J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[120,160)forC1C1WWgrid">SR-DF-0J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[100,105)forC1C1WWgrid">SR-DF-0J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[105,110)forC1C1WWgrid">SR-DF-0J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[110,120)forC1C1WWgrid">SR-DF-0J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[120,140)forC1C1WWgrid">SR-DF-0J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[140,160)forC1C1WWgrid">SR-DF-0J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[160,180)forC1C1WWgrid">SR-DF-0J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[180,220)forC1C1WWgrid">SR-DF-0J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[220,260)forC1C1WWgrid">SR-DF-0J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-DF-0J-[260,inf)forC1C1WWgrid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,inf)forC1C1WWgrid">SR-DF-1J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[160,inf)forC1C1WWgrid">SR-DF-1J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,120)forC1C1WWgrid">SR-DF-1J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[120,160)forC1C1WWgrid">SR-DF-1J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[100,105)forC1C1WWgrid">SR-DF-1J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[105,110)forC1C1WWgrid">SR-DF-1J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[110,120)forC1C1WWgrid">SR-DF-1J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[120,140)forC1C1WWgrid">SR-DF-1J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[140,160)forC1C1WWgrid">SR-DF-1J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[160,180)forC1C1WWgrid">SR-DF-1J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[180,220)forC1C1WWgrid">SR-DF-1J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[220,260)forC1C1WWgrid">SR-DF-1J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-DF-1J-[260,inf)forC1C1WWgrid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,inf)forC1C1WWgrid">SR-SF-0J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[160,inf)forC1C1WWgrid">SR-SF-0J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,120)forC1C1WWgrid">SR-SF-0J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[120,160)forC1C1WWgrid">SR-SF-0J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[100,105)forC1C1WWgrid">SR-SF-0J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[105,110)forC1C1WWgrid">SR-SF-0J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[110,120)forC1C1WWgrid">SR-SF-0J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[120,140)forC1C1WWgrid">SR-SF-0J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[140,160)forC1C1WWgrid">SR-SF-0J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[160,180)forC1C1WWgrid">SR-SF-0J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[180,220)forC1C1WWgrid">SR-SF-0J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[220,260)forC1C1WWgrid">SR-SF-0J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-SF-0J-[260,inf)forC1C1WWgrid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,inf)forC1C1WWgrid">SR-SF-1J-[100,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[160,inf)forC1C1WWgrid">SR-SF-1J-[160,inf) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,120)forC1C1WWgrid">SR-SF-1J-[100,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[120,160)forC1C1WWgrid">SR-SF-1J-[120,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[100,105)forC1C1WWgrid">SR-SF-1J-[100,105) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[105,110)forC1C1WWgrid">SR-SF-1J-[105,110) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[110,120)forC1C1WWgrid">SR-SF-1J-[110,120) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[120,140)forC1C1WWgrid">SR-SF-1J-[120,140) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[140,160)forC1C1WWgrid">SR-SF-1J-[140,160) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[160,180)forC1C1WWgrid">SR-SF-1J-[160,180) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[180,220)forC1C1WWgrid">SR-SF-1J-[180,220) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[220,260)forC1C1WWgrid">SR-SF-1J-[220,260) </a> <a href="89413?version=1&table=EfficiencySR-SF-1J-[260,inf)forC1C1WWgrid">SR-SF-1J-[260,inf) </a><br/> </ul> <b>Cutflow:</b> <ul> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct chargino-pair production via W decay $m(\tilde{\chi}^{\pm}_1,\tilde{\chi}^{0}_1)=(300,50) GeV$</a> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct chargino-pair production via slepton decay $m(\tilde{\chi}^{\pm}_1,\tilde{l},\tilde{\chi}^{0}_1)=(600,300,1) GeV$</a> <li><a href="89413?version=1&table=Cutflow1">Cutflow for direct slepton-pair production $m(\tilde{l},\tilde{\chi}^{0}_1)=(400,200) GeV$</a> </ul> <b>SimpleAnalysis framework implementation</b> of the search SRs is available under "Resources" (purple button on the left)
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Background Fit results:</b> <ul> <li><a href="89413?version=3&table=Background fit 1">CRs</a> <li><a href="89413?version=3&table=Background fit 2">VRs</a> <li><a href="89413?version=3&table=Background fit 5">inclusive DF-0J SRs</a> <li><a href="89413?version=3&table=Background fit 6">inclusive DF-1J SRs</a> <li><a href="89413?version=3&table=Background fit 3">inclusive SF-0J SRs</a> <li><a href="89413?version=3&table=Background fit 4">inclusive SF-1J SRs</a> </ul> <b>Kinematic distributions in VRs:</b> <ul> <li><a href="89413?version=3&table=VR kinematics 1">$m_{T2}$ in VR-top-low</a> <li><a href="89413?version=3&table=VR kinematics 2">$m_{T2}$ in VR-top-high</a> <li><a href="89413?version=3&table=VR kinematics 3">$E_T^{miss}$ in VR-WW-0J</a> <li><a href="89413?version=3&table=VR kinematics 4">$E_T^{miss}$ in VR-WW-1J</a> <li><a href="89413?version=3&table=VR kinematics 5">$E_T^{miss}$ sig in VR-VZ</a> <li><a href="89413?version=3&table=VR kinematics 6">$E_T^{miss}$ sig in VR-top-WW</a> </ul> <b>Kinematic distributions in SRs:</b> <ul> <li><a href="89413?version=3&table=SR kinematics 1">$m_{T2}$ in SR-SF-0J</a> <li><a href="89413?version=3&table=SR kinematics 2">$m_{T2}$ in SR-SF-1J</a> <li><a href="89413?version=3&table=SR kinematics 3">$m_{T2}$ in SR-DF-0J</a> <li><a href="89413?version=3&table=SR kinematics 4">$m_{T2}$ in SR-DF-1J</a> </ul> <b>Systematic uncertaities:</b> <ul> <li><a href="89413?version=3&table=Systematic uncertainties">dominant systematic uncertainties in the inclusive SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=3&table=Exclusion contour (exp) 1">expected exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 1">observed exclusion contour direct chargino-pair production via W decay grid</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 2">expected exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 2">observed exclusion contour direct chargino-pair production via slepton decay grid</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 3">expected exclusion contour direct slepton-pair production grid</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 3">observed exclusion contour direct slepton-pair production grid</a> </ul> <br/><br/><b>AUXILIARY MATERIAL</b><br/> <b>Background Fit in binned SRs:</b> <ul> <li><a href="89413?version=3&table=Background fit 7">binned DF-0J SRs</a> <li><a href="89413?version=3&table=Background fit 8">binned DF-1J SRs</a> <li><a href="89413?version=3&table=Background fit 9">binned SF-0J SRs</a> <li><a href="89413?version=3&table=Background fit 10">binned SF-1J SRs</a> </ul> <b>Exclusion contours:</b> <ul> <li><a href="89413?version=3&table=Exclusion contour (exp) 4">expected exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 4">observed exclusion contour left-handed slepton-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 5">expected exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 5">observed exclusion contour right-handed slepton-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 6">expected exclusion contour selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 6">observed exclusion contour selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 7">expected exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 7">observed exclusion contour left-handed selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 8">expected exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 8">observed exclusion contour right-handed selectron-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 9">expected exclusion contour smuon-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 9">observed exclusion contour smuon-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 10">expected exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 10">observed exclusion contour left-handed smuon-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (exp) 11">expected exclusion contour right-handed smuon-pair production</a> <li><a href="89413?version=3&table=Exclusion contour (obs) 11">observed exclusion contour right-handed smuon-pair production</a> </ul> <b>Cross section upper limits:</b> <ul> <li><a href="89413?version=3&table=xsec upper limits 1">upper limits on signal cross section for direct chargino-pair production via W decay</a> <li><a href="89413?version=3&table=xsec upper limits 2">upper limits on signal cross section for direct chargino-pair production via slepton decay</a> <li><a href="89413?version=3&table=xsec upper limits 3">upper limits on signal cross section for direct slepton-pair production</a> </ul> <b>Acceptances and Efficiencies for direct chargino-pair production via W decay grid </b> <ul> <li> <b>Acceptance</b> <br/> <a href="89413?version=3&table=Acceptance SR-DF-0J-[100,inf) for C1C1WW grid">SR-DF-0J-[100,inf) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[160,inf) for C1C1WW grid">SR-DF-0J-[160,inf) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[100,120) for C1C1WW grid">SR-DF-0J-[100,120) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[120,160) for C1C1WW grid">SR-DF-0J-[120,160) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[100,105) for C1C1WW grid">SR-DF-0J-[100,105) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[105,110) for C1C1WW grid">SR-DF-0J-[105,110) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[110,120) for C1C1WW grid">SR-DF-0J-[110,120) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[120,140) for C1C1WW grid">SR-DF-0J-[120,140) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[140,160) for C1C1WW grid">SR-DF-0J-[140,160) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[160,180) for C1C1WW grid">SR-DF-0J-[160,180) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[180,220) for C1C1WW grid">SR-DF-0J-[180,220) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[220,260) for C1C1WW grid">SR-DF-0J-[220,260) </a> <a href="89413?version=3&table=Acceptance SR-DF-0J-[260,inf) for C1C1WW grid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=3&table=Acceptance SR-DF-1J-[100,inf) for C1C1WW grid">SR-DF-1J-[100,inf) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[160,inf) for C1C1WW grid">SR-DF-1J-[160,inf) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[100,120) for C1C1WW grid">SR-DF-1J-[100,120) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[120,160) for C1C1WW grid">SR-DF-1J-[120,160) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[100,105) for C1C1WW grid">SR-DF-1J-[100,105) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[105,110) for C1C1WW grid">SR-DF-1J-[105,110) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[110,120) for C1C1WW grid">SR-DF-1J-[110,120) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[120,140) for C1C1WW grid">SR-DF-1J-[120,140) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[140,160) for C1C1WW grid">SR-DF-1J-[140,160) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[160,180) for C1C1WW grid">SR-DF-1J-[160,180) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[180,220) for C1C1WW grid">SR-DF-1J-[180,220) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[220,260) for C1C1WW grid">SR-DF-1J-[220,260) </a> <a href="89413?version=3&table=Acceptance SR-DF-1J-[260,inf) for C1C1WW grid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=3&table=Acceptance SR-SF-0J-[100,inf) for C1C1WW grid">SR-SF-0J-[100,inf) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[160,inf) for C1C1WW grid">SR-SF-0J-[160,inf) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[100,120) for C1C1WW grid">SR-SF-0J-[100,120) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[120,160) for C1C1WW grid">SR-SF-0J-[120,160) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[100,105) for C1C1WW grid">SR-SF-0J-[100,105) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[105,110) for C1C1WW grid">SR-SF-0J-[105,110) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[110,120) for C1C1WW grid">SR-SF-0J-[110,120) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[120,140) for C1C1WW grid">SR-SF-0J-[120,140) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[140,160) for C1C1WW grid">SR-SF-0J-[140,160) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[160,180) for C1C1WW grid">SR-SF-0J-[160,180) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[180,220) for C1C1WW grid">SR-SF-0J-[180,220) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[220,260) for C1C1WW grid">SR-SF-0J-[220,260) </a> <a href="89413?version=3&table=Acceptance SR-SF-0J-[260,inf) for C1C1WW grid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=3&table=Acceptance SR-SF-1J-[100,inf) for C1C1WW grid">SR-SF-1J-[100,inf) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[160,inf) for C1C1WW grid">SR-SF-1J-[160,inf) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[100,120) for C1C1WW grid">SR-SF-1J-[100,120) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[120,160) for C1C1WW grid">SR-SF-1J-[120,160) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[100,105) for C1C1WW grid">SR-SF-1J-[100,105) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[105,110) for C1C1WW grid">SR-SF-1J-[105,110) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[110,120) for C1C1WW grid">SR-SF-1J-[110,120) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[120,140) for C1C1WW grid">SR-SF-1J-[120,140) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[140,160) for C1C1WW grid">SR-SF-1J-[140,160) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[160,180) for C1C1WW grid">SR-SF-1J-[160,180) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[180,220) for C1C1WW grid">SR-SF-1J-[180,220) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[220,260) for C1C1WW grid">SR-SF-1J-[220,260) </a> <a href="89413?version=3&table=Acceptance SR-SF-1J-[260,inf) for C1C1WW grid">SR-SF-1J-[260,inf) </a><br/> <li> <b>Efficiency</b> <br/> <a href="89413?version=3&table=Efficiency SR-DF-0J-[100,inf) for C1C1WW grid">SR-DF-0J-[100,inf) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[160,inf) for C1C1WW grid">SR-DF-0J-[160,inf) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[100,120) for C1C1WW grid">SR-DF-0J-[100,120) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[120,160) for C1C1WW grid">SR-DF-0J-[120,160) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[100,105) for C1C1WW grid">SR-DF-0J-[100,105) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[105,110) for C1C1WW grid">SR-DF-0J-[105,110) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[110,120) for C1C1WW grid">SR-DF-0J-[110,120) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[120,140) for C1C1WW grid">SR-DF-0J-[120,140) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[140,160) for C1C1WW grid">SR-DF-0J-[140,160) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[160,180) for C1C1WW grid">SR-DF-0J-[160,180) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[180,220) for C1C1WW grid">SR-DF-0J-[180,220) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[220,260) for C1C1WW grid">SR-DF-0J-[220,260) </a> <a href="89413?version=3&table=Efficiency SR-DF-0J-[260,inf) for C1C1WW grid">SR-DF-0J-[260,inf) </a><br/> <a href="89413?version=3&table=Efficiency SR-DF-1J-[100,inf) for C1C1WW grid">SR-DF-1J-[100,inf) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[160,inf) for C1C1WW grid">SR-DF-1J-[160,inf) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[100,120) for C1C1WW grid">SR-DF-1J-[100,120) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[120,160) for C1C1WW grid">SR-DF-1J-[120,160) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[100,105) for C1C1WW grid">SR-DF-1J-[100,105) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[105,110) for C1C1WW grid">SR-DF-1J-[105,110) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[110,120) for C1C1WW grid">SR-DF-1J-[110,120) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[120,140) for C1C1WW grid">SR-DF-1J-[120,140) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[140,160) for C1C1WW grid">SR-DF-1J-[140,160) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[160,180) for C1C1WW grid">SR-DF-1J-[160,180) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[180,220) for C1C1WW grid">SR-DF-1J-[180,220) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[220,260) for C1C1WW grid">SR-DF-1J-[220,260) </a> <a href="89413?version=3&table=Efficiency SR-DF-1J-[260,inf) for C1C1WW grid">SR-DF-1J-[260,inf) </a><br/> <a href="89413?version=3&table=Efficiency SR-SF-0J-[100,inf) for C1C1WW grid">SR-SF-0J-[100,inf) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[160,inf) for C1C1WW grid">SR-SF-0J-[160,inf) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[100,120) for C1C1WW grid">SR-SF-0J-[100,120) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[120,160) for C1C1WW grid">SR-SF-0J-[120,160) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[100,105) for C1C1WW grid">SR-SF-0J-[100,105) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[105,110) for C1C1WW grid">SR-SF-0J-[105,110) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[110,120) for C1C1WW grid">SR-SF-0J-[110,120) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[120,140) for C1C1WW grid">SR-SF-0J-[120,140) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[140,160) for C1C1WW grid">SR-SF-0J-[140,160) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[160,180) for C1C1WW grid">SR-SF-0J-[160,180) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[180,220) for C1C1WW grid">SR-SF-0J-[180,220) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[220,260) for C1C1WW grid">SR-SF-0J-[220,260) </a> <a href="89413?version=3&table=Efficiency SR-SF-0J-[260,inf) for C1C1WW grid">SR-SF-0J-[260,inf) </a><br/> <a href="89413?version=3&table=Efficiency SR-SF-1J-[100,inf) for C1C1WW grid">SR-SF-1J-[100,inf) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[160,inf) for C1C1WW grid">SR-SF-1J-[160,inf) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[100,120) for C1C1WW grid">SR-SF-1J-[100,120) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[120,160) for C1C1WW grid">SR-SF-1J-[120,160) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[100,105) for C1C1WW grid">SR-SF-1J-[100,105) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[105,110) for C1C1WW grid">SR-SF-1J-[105,110) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[110,120) for C1C1WW grid">SR-SF-1J-[110,120) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[120,140) for C1C1WW grid">SR-SF-1J-[120,140) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[140,160) for C1C1WW grid">SR-SF-1J-[140,160) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[160,180) for C1C1WW grid">SR-SF-1J-[160,180) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[180,220) for C1C1WW grid">SR-SF-1J-[180,220) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[220,260) for C1C1WW grid">SR-SF-1J-[220,260) </a> <a href="89413?version=3&table=Efficiency SR-SF-1J-[260,inf) for C1C1WW grid">SR-SF-1J-[260,inf) </a><br/> </ul> <b>Cutflow:</b> <ul> <li><a href="89413?version=3&table=Cutflow 1">Cutflow for direct chargino-pair production via W decay $m(\tilde{\chi}^{\pm}_1,\tilde{\chi}^{0}_1)=(300,50) GeV$</a> <li><a href="89413?version=3&table=Cutflow 2">Cutflow for direct chargino-pair production via slepton decay $m(\tilde{\chi}^{\pm}_1,\tilde{l},\tilde{\chi}^{0}_1)=(600,300,1) GeV$</a> <li><a href="89413?version=3&table=Cutflow 3">Cutflow for direct slepton-pair production $m(\tilde{l},\tilde{\chi}^{0}_1)=(400,200) GeV$</a> </ul> <b>SimpleAnalysis framework implementation</b> of the search SRs is available under "Resources" (purple button on the left)
To assess the properties of the quark-gluon plasma formed in heavy-ion collisions, the ATLAS experiment at the LHC measures a correlation between the mean transverse momentum and the magnitudes of the flow harmonics. The analysis uses data samples of lead-lead and proton-lead collisions obtained at the centre-of-mass energy per nucleon pair of 5.02 TeV, corresponding to total integrated luminosities of $22 ~\mu b^{-1}$ and $28~nb^{-1}$, respectively. The measurement is performed using a modified Pearson correlation coefficient with the charged-particle tracks on an event-by-event basis. The modified Pearson correlation coefficients for the $2^{nd}$-, 3$^{rd}$-, and 4$^{th}$-order harmonics are measured as a function of event centrality quantified as the number of charged particles or the number of nucleons participating in the collision. The measurements are performed for several intervals of the charged-particle transverse momentum. The correlation coefficients for all studied harmonics exhibit a strong centrality evolution in the lead-lead collisions, which only weakly depends on the charged-particle momentum range. In the proton-lead collisions, the modified Pearson correlation coefficient measured for the second harmonics shows only weak centrality dependence. The data is qualitatively described by the predictions based on the hydrodynamical model.
The $cov(v_{3}^{2},[p_{T}])$ for Pb+Pb collisions for the $p_T$ 0.5-2 GeV interval as a function $N_{ch}$.
A search for Higgs boson pair production via vector-boson fusion (VBF) in the $b\bar{b}b\bar{b}$ final state is carried out with the ATLAS experiment using 126 fb$^{-1}$ of proton-proton collision data delivered at $\sqrt{s} = 13$ TeV by the Large Hadron Collider. This search is sensitive to VBF production of additional heavy bosons that may decay into Higgs boson pairs, and in a non-resonant topology it can constrain the quartic coupling between the Higgs bosons and vector bosons. No significant excess relative to the Standard Model expectation is observed, and limits on the production cross-section are set at the 95 % confidence level for a heavy scalar resonance in the context of an extended Higgs sector, and for non-resonant Higgs boson pair production. Interpretation in terms of the coupling between a Higgs boson pair and two vector bosons is also provided: coupling values normalised to the Standard Model expectation of $\kappa_{2V} < -0.43$ and $\kappa_{2V} > 2.56$ are excluded at the 95 % confidence level in data.
Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.
Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.
Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.
An observation of electroweak $W^{\pm}Z$ production in association with two jets in proton-proton collisions is presented. The data collected by the ATLAS detector at the Large Hadron Collider in 2015 and 2016 at a centre-of-mass energy of $\sqrt{s} =$ 13 TeV are used, corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Events containing three identified leptons, either electrons or muons, and two jets are selected. The electroweak production of $W^{\pm}Z$ bosons in association with two jets is measured with an observed significance of 5.3 standard deviations. A fiducial cross-section for electroweak production including interference effects is measured to be $\sigma_{WZjj\mathrm{-EW}} = 0.57 \; ^{+ 0.14} _{- 0.13} \,(\mathrm{stat.}) \; ^{+ 0.07} _{- 0.06} \,(\mathrm{syst.}) \; \mathrm{fb}$. Total and differential fiducial cross-sections of the sum of $W^\pm Z jj$ electroweak and strong productions for several kinematic observables are also measured.
Fiducial cross section of the electroweak $W^{\pm}Z$ boson pair production in association with two jets. The first systematic uncertainty is experimental, the second is the theory modelling and interference systematics and the third one is the luminosity uncertainty.
Fiducial cross section of the $W^{\pm}Z$ boson pair production in association with two jets. The first systematic uncertainty is experimental, the second is the theory modelling and interference systematics and the third one is the luminosity uncertainty.
A measurement of the four-lepton invariant mass spectrum is made with the ATLAS detector, using an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$ = 13 TeV delivered by the Large Hadron Collider. The differential cross-section is measured for events containing two same-flavour opposite-sign lepton pairs. It exhibits a rich structure, with different mass regions dominated in the Standard Model by single $Z$ boson production, Higgs boson production, and $Z$ boson pair production, and non-negligible interference effects at high invariant masses. The measurement is compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. These calculations are used to interpret the data in terms of $gg\rightarrow ZZ \rightarrow 4\ell$ and $Z \rightarrow 4\ell$ subprocesses, and to place constraints on a possible contribution from physics beyond the Standard Model.
Measured and expected differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$
Measured and expected differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 0$< p_{T}^{4l} <$20 GeV
Measured and expected differential cross-section $\text{d}\sigma / \text{d} m_{4l}$ as a function of $m_{4l}$ in bin of 20$< p_{T}^{4l} <$50 GeV
A search for a new $Z'$ gauge boson predicted by $L_{\mu}-L_{\tau}$ models, based on charged-current Drell-Yan production, $pp \rightarrow W^{\pm(*)} \rightarrow Z' \mu^{\pm} \nu \rightarrow \mu^{\pm}\mu^{\mp}\mu^{\pm}\nu$, is presented. The data sample used corresponds to an integrated luminosity of 140 fb$^{-1}$ of proton-proton collisions at $\sqrt{s} = 13$ TeV recorded by the ATLAS detector at the Large Hadron Collider. The search examines a final state of $3\mu$ plus large missing transverse momentum. Upper limits are set on the $Z'$ production cross-section times branching ratio in the mass range of 5-81 GeV. After combining with the previous $Z'$ search using the neutral-current Drell-Yan production with a $4\mu$ final state, the most stringent exclusion limits to date are achieved in the parameter space of the $Z'$ coupling strength and mass.
Observed and expected upper limits at 95% CL on the production cross-section times branching fraction of the process $pp\to W\to Z^{\prime}$ $\mu \nu \to \mu \mu \mu \nu$ as a function of $m_{Z^{\prime}}$.
We have measured the inclusive production of J ψ in 16 and 22 GeV π − copper collisions in a wide aperture magnetic spectrometer. The cross section per Cu nucleus for x > 0 corrected for branching ratio is 64 ± 38 nb at 16 GeV and 196 ± 38 nb at 22 GeV. As threshold is approached, the mean values of the Feynman x distribution increase and the cross section for J ψ production drops steeply. This can be understood in terms of the quark-fusion model where the antiquark content of the pion makes an increasingly significant contribution as M 2 s increases.
A search for resonant and non-resonant pair production of Higgs bosons in the $b\bar{b}\tau^+\tau^-$ final state is presented. The search uses 36.1 fb$^{-1}$ of $pp$ collision data with $\sqrt{s}= 13$ TeV recorded by the ATLAS experiment at the LHC in 2015 and 2016. The semileptonic and fully hadronic decays of the $\tau$-lepton pair are considered. No significant excess above the expected background is observed in the data. The cross-section times branching ratio for non-resonant Higgs boson pair production is constrained to be less than 30.9 fb, 12.7 times the Standard Model expectation, at 95% confidence level. The data are also analyzed to probe resonant Higgs boson pair production, constraining a model with an extended Higgs sector based on two doublets and a Randall-Sundrum bulk graviton model. Upper limits are placed on the resonant Higgs boson pair production cross-section times branching ratio, excluding resonances $X$ in the mass range $305~{\rm GeV} < m_X < 402~{\rm GeV}$ in the simplified hMSSM minimal supersymmetric model for $\tan\beta=2$ and excluding bulk Randall-Sundrum gravitons $G_{\mathrm{KK}}$ in the mass range $325~{\rm GeV} < m_{G_{\mathrm{KK}}} < 885~{\rm GeV}$ for $k/\overline{M}_{\mathrm{Pl}} = 1$.
Upper limits on the production cross-section times the HH to bbtautau branching ratio for non-resonant HH at 95% CLS and their interpretation as multiples of the SM prediction
Upper limits on the production cross-section times the HH to bbtautau branching ratio divided by the SM prediction for non-resonant HH at 95% CL
This letter presents a combination of searches for Higgs boson pair production using up to 36.1 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy $\sqrt{s} = 13$ TeV recorded with the ATLAS detector at the LHC. The combination is performed using six analyses searching for Higgs boson pairs decaying into the bbbb, bbWW, bb$\tau\tau$, WWWW, bb$\gamma \gamma$ and WW$\gamma\gamma$ final states. Results are presented for non-resonant and resonant Higgs boson pair production modes. No statistically significant excess in data above the Standard Model predictions is found. The combined observed (expected) limit at 95% confidence level on the non-resonant Higgs boson pair production cross-section is 6.9 (10) times the predicted Standard Model cross-section. Limits are also set on the ratio ($ \kappa_{\lambda} $) of the Higgs boson self-coupling to its Standard Model value. This ratio is constrained at 95% confidence level in observation (expectation) to $ -5.0 < \kappa_{\lambda} <12.0 $ ($ -5.8 < \kappa_{\lambda} <12.0 $). In addition, limits are set on the production of narrow scalar resonances and spin-2 Kaluza-Klein Randall-Sundrum gravitons. Exclusion regions are also provided in the parameter space of the habemus Minimal Supersymmetric Standard Model and the Electroweak Singlet Model.
Signal acceptance times efficiency as a function of κ<sub>λ</sub> for the $b\bar{b}b\bar{b}$, $b\bar{b}\tau^{+}\tau^{-}$ and $b\bar{b}\gamma\gamma$ analyses. The $b\bar{b}b\bar{b}$ curve is the average of the 2015 and 2016 curves weighted by the integrated luminosities of the two datasets
Upper limits at 95% CL on the cross-section of the ggF non-resonant SM HH production as a function of κ<sub>λ</sub>. The observed (expected) limits are shown as solid (dashed) lines. In the $b\bar{b}\gamma\gamma$ final state, the observed and expected limits coincide. The $\pm 1 \sigma$ and $\pm 2\sigma$ bands are only shown for the combined expected limit. The theoretical prediction of the cross-section as a function of κ<sub>λ</sub> is also shown.
Upper limits at 95% CL on the cross-section of the resonant Higgs boson pair production for a spin-0 heavy scalar
Measurements of energy weighted angular correlations in electron positron annihilations at c.m. energies of 22 GeV and 34 GeV are presented.
Based on a sample of 22 four-prong D 0 / D 0 decays produced in hydrogen by 360 GeV/ c π − , we present the following new results: mean lifetime τ = (3.5 −0.9 +1.4 ) x 10 −13 s ; production cross section for x F > 0.0, σ = (10.3 ± 3.5) ωb ; the D → K ± π ± π + π − branching ratio = (7.1 ± 2.5)%.
No description provided.
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 search for non-resonant Higgs boson pair production, as predicted by the Standard Model, is presented, where one of the Higgs bosons decays via the $H\rightarrow bb$ channel and the other via one of the $H \rightarrow WW^*/ZZ^*/\tau\tau$ channels. The analysis selection requires events to have at least two $b$-tagged jets and exactly two leptons (electrons or muons) with opposite electric charge in the final state. Candidate events consistent with Higgs boson pair production are selected using a multi-class neural network discriminant. The analysis uses 139 fb$^{-1}$ of $pp$ collision data recorded at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. An observed (expected) upper limit of 1.2 ($0.9^{+0.4}_{-0.3}$) pb is set on the non-resonant Higgs boson pair production cross-section at 95% confidence level, which is equivalent to 40 ($29^{+14}_{-9}$) times the value predicted in the Standard Model.
Expected and observed $95\%$ CL limits on the cross-section of ggF non-resonant Higgs boson pair production as a function of the Higgs boson self-coupling modifier, $\kappa_{\lambda} = \lambda_{HHH} / \lambda_{HHH}^{\textit{SM}}$. The $\pm 1 \sigma$ and $\pm 2 \sigma$ variations about the expected limit, due to statistical and systematic uncertainties, are also shown. The method used for producing estimates of $HH$ production at non-SM values of $\kappa_{\lambda}$ is fully described in arXiv:1906.02025. The theory prediction curve represents the scenario where all parameters and couplings are set to their SM values except for $\kappa_{\lambda}$, also described in arXiv:1906.02025. The uncertainty band on the theory prediction indicates the theoretical uncertainty of this prediction. No additional analysis optimisation relative to that appearing in the main body of the analysis is performed to become particularly sensitive to non-SM values of $\kappa_{\lambda}$. The vertical dashed line indicates the SM scenario with $\kappa_{\lambda} = 1$.
Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the $b\bar{b}b\bar{b}$, $b\bar{b}\tau^+\tau^-$ and $b\bar{b} \gamma \gamma$ decay channels with single-Higgs boson analyses targeting the $\gamma \gamma$, $ZZ^*$, $WW^*$, $\tau^+ \tau^-$ and $b\bar{b}$ decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton$-$proton collisions at $\sqrt{s}=13$ TeV and correspond to an integrated luminosity of 126$-$139 fb$^{-1}$. The combination of the double-Higgs analyses sets an upper limit of $\mu_{HH} < 2.4$ at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling ($\lambda_{HHH}$), values outside the interval $-0.4< \kappa_{\lambda}=(\lambda_{HHH}/\lambda_{HHH}^{\textrm{SM}})< 6.3$ are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles. In this relaxed scenario, the constraint becomes $-1.4 < \kappa_{\lambda} < 6.1$ at 95% CL.
Observed and expected 95% CL upper limits on the signal strength for double-Higgs production from the bbbb, bb$\tau\tau$ and bb$\gamma\gamma$ decay channels, and their statistical combination. The value $m_H$ = 125.09 GeV is assumed when deriving the predicted SM cross-section. The expected limit and the corresponding error bands are derived assuming the absence of the HH process and with all nuisance parameters profiled to the observed data.
Observed and expected 95% CL exclusion limits on the production cross-sections of the combined ggF HH and VBF HH processes as a function of $\kappa_\lambda$, for the three double-Higgs search channels and their combination. The expected limits assume no HH production. The red line shows the theory prediction for the combined ggF HH and VBF HH cross-section as a function of $\kappa_\lambda$ where all parameters and couplings are set to their SM values except for $\kappa_\lambda$. The band surrounding the red cross-section lines indicate the theoretical uncertainty of the predicted cross-section.
Observed and expected 95% CL exclusion limits on the production cross-sections of the VBF HH process as a function of $\kappa_{2V}$, for the three double-Higgs search channels and their combination. The expected limits assume no VBF HH production. The red line shows the predicted VBF HH cross-section as a function of $\kappa_{2V}$. The bands surrounding the red cross-section lines indicate the theoretical uncertainty of the predicted cross-section. The uncertainty band is smaller than the width of the plotted line.
The production of $W^{\pm}Z$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb$^{-1}$. The $W^{\pm}Z$ candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is $\sigma_{W^\pm Z \rightarrow \ell^{'} \nu \ell \ell}^{\textrm{fid.}} = 63.2 \pm 3.2$ (stat.) $\pm 2.6$ (sys.) $\pm 1.5$ (lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is $53.4^{+3.6}_{-2.8}$ fb. The extrapolation of the measurement from the fiducial to the total phase space yields $\sigma_{W^{\pm}Z}^{\textrm{tot.}} = 50.6 \pm 2.6$ (stat.) $\pm 2.0$ (sys.) $\pm 0.9$ (th.) $\pm 1.2$ (lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of $48.2^{+1.1}_{-1.0}$ pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent $W^+Z$ and $W^-Z$ cross sections and their ratio.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of $\sqrt{s} = $13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing $b$-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical $Z'$ bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross-sections, the $Z'$ boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1$-$3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 TeV to 0.9 TeV and from 2.0 TeV to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.
Expected and observed upper limits on cross-section times branching fraction of Kaluza-Klein gluon decaying into top-quark pair as a function of the width of Kaluza-Klein gluon for masses of 1 TeV.
A measurement of $W^\pm$ boson production in lead-lead collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV is reported using data recorded by the ATLAS experiment at the LHC in 2015, corresponding to a total integrated luminosity of $0.49\;\mathrm{nb^{-1}}$. The $W^\pm$ bosons are reconstructed in the electron or muon leptonic decay channels. Production yields of leptonically decaying $W^\pm$ bosons, normalised by the total number of minimum-bias events and the nuclear thickness function, are measured within a fiducial region defined by the detector acceptance and the main kinematic requirements. These normalised yields are measured separately for $W^+$ and $W^-$ bosons, and are presented as a function of the absolute value of pseudorapidity of the charged lepton and of the collision centrality. The lepton charge asymmetry is also measured as a function of the absolute value of lepton pseudorapidity. In addition, nuclear modification factors are calculated using the $W^\pm$ boson production cross-sections measured in $pp$ collisions. The results are compared with predictions based on next-to-leading-order calculations with CT14 parton distribution functions as well as with predictions obtained with the EPPS16 and nCTEQ15 nuclear parton distribution functions. No dependence of normalised production yields on centrality and a good agreement with predictions are observed for mid-central and central collisions. For peripheral collisions, the data agree with predictions within 1.7 (0.9) standard deviations for $W^-$ ($W^+$) bosons.
Differential normalised production yields for $W^+$ bosons as a function of absolute pseudorapidity of the charged lepton for the combined electron and muon channels. Systematic uncertainties related to $T_{\mathrm{AA}}$ are not included.
Differential normalised production yields for $W^-$ bosons as a function of absolute pseudorapidity of the charged lepton for the combined electron and muon channels. Systematic uncertainties related to $T_{\mathrm{AA}}$ are not included.
Normalised production yields of $W^+$ and $W^-$ bosons as a function of $⟨N_{\mathrm{part}}⟩$ shown for the combination of electron and muon decay channels.
A combination of searches for resonant Higgs boson pair production is presented, using up to 139 fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=13$ TeV recorded with the ATLAS detector at the LHC. The combination includes searches performed in three decay channels: $b\bar{b}b\bar{b}$, $bb\tau^+\tau^-$ and $bb\gamma\gamma$. No excess above the expected background is observed and upper limits are set at the 95% confidence level on the production cross section of Higgs boson pairs originating from the decay of a narrow scalar resonance with mass in the range 251 GeV-5 TeV. The observed (expected) limits are in the range 0.96-600 fb (1.2-390 fb). The limits are interpreted in the Type-I Two-Higgs-Doublet Model and the Minimimal Supersymmetric Standard Model, and constrain parameter space not previously excluded by other searches.
Local p-value as a function of the resonance mass $m_{X}$. Some table entries are empty because resonance masses from 251 GeV to 5 TeV are considered, whereas some channels only use masses in a certain, more restricted, range.
Observed significance as a function of the resonance $m_{X}$. Some table entries are empty because resonance masses from 251 GeV to 5 TeV are considered, whereas some channels only use masses in a certain, more restricted, range.
Observed and expected upper limits at the 95% CL on the resonant Higgs boson pair production cross section as a function of the resonance mass $m_{X}$. Some table entries are empty because resonance masses from 251 GeV to 5 TeV are considered, whereas some channels only use masses in a certain, more restricted, range.
A search is conducted for the electroweak pair production of a chargino and a neutralino $pp \rightarrow \tilde\chi^\pm_1 \tilde\chi^0_2$, where the chargino decays into the lightest neutralino and a $W$ boson, $\tilde\chi^\pm_1 \rightarrow \tilde\chi^0_1 W^{\pm}$, while the neutralino decays into the lightest neutralino and a Standard Model-like 125 GeV Higgs boson, $\tilde\chi^0_2 \rightarrow \tilde\chi^0_1 h$. Fully hadronic, semileptonic, diphoton, and multilepton (electrons, muons) final states with missing transverse momentum are considered in this search. Higgs bosons in the final state are identified by either two jets originating from bottom quarks ($h \rightarrow b\bar{b}$), two photons ($h \rightarrow \gamma\gamma$), or leptons from the decay modes $h \rightarrow WW$, $h \rightarrow ZZ$ or $h \rightarrow \tau \tau$. The analysis is based on 36.1 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. Observations are consistent with the Standard Model expectations, and 95% confidence-level limits of up to 680 GeV in $\tilde\chi^\pm_1/\tilde\chi^0_2$ mass are set in the context of a simplified supersymmetric model.
Acceptance for $0lb\bar{b}$ SRHad-Low signal region. Note that the acceptance is relative to the total chargino-neutralino production cross section.
Acceptance for $0lb\bar{b}$ SRHad-High signal region. Note that the acceptance is relative to the total chargino-neutralino production cross section.
Acceptance for $1lb\bar{b}$ SR1Lbb-Low signal region. Note that the acceptance is relative to the total chargino-neutralino production cross section.
A search for vectorlike quarks is presented, which targets their decay into a $Z$ boson and a third-generation Standard Model quark. In the case of a vectorlike quark $T$ ($B$) with charge $+2/3e$ ($-1/3e$), the decay searched for is $T \rightarrow Zt$ ($B \rightarrow Zb$). Data for this analysis were taken during 2015 and 2016 with the ATLAS detector at the Large Hadron Collider and correspond to an integrated luminosity of 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV. The final state used is characterized by the presence of $b$-tagged jets, as well as a $Z$ boson with high transverse momentum, which is reconstructed from a pair of opposite-sign same-flavor leptons. Pair and single production of vectorlike quarks are both taken into account and are each searched for using optimized dileptonic exclusive and trileptonic inclusive event selections. In these selections, the high scalar sum of jet transverse momenta, the presence of high-transverse-momentum large-radius jets, as well as - in the case of the single-production selections - the presence of forward jets are used. No significant excess over the background-only hypothesis is found and exclusion limits at 95% confidence level allow masses of vectorlike quarks of $m_T > 1030$ GeV ($m_T > 1210$ GeV) and $m_B > 1010$ GeV ($m_B > 1140$ GeV) in the singlet (doublet) model. In the case of 100% branching ratio for $T\rightarrow Zt$ ($B\rightarrow Zb$), the limits are $m_T > 1340$ GeV ($m_B > 1220$ GeV). Limits at 95% confidence level are also set on the coupling to Standard Model quarks for given vectorlike quark masses.
Comparison of the distribution of the scalar sum of small-$R$ jet transverse momenta, $H_T$, between data and the background prediction in the 0-large-$R$ jet-signal region of the pair-production (PP) $2\ell$ $0-1$J channel. The background prediction is shown post-fit, i.e. after the fit to the data $H_T$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a $B\bar B$ signal in the singlet model with $m_B$ = 900 GeV is overlaid.
Comparison of the distribution of the scalar sum of small-$R$ jet transverse momenta, $H_T$, between data and the background prediction in the 1-large-$R$ jet-signal region of the pair-production (PP) $2\ell$ $0-1$J channel. The background prediction is shown post-fit, i.e. after the fit to the data $H_T$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a $B\bar B$ signal in the singlet model with $m_B$ = 900 GeV is overlaid.
Comparison of the distribution of the invariant mass of the $Z$ boson candidate and the highest-$p_T$ $b$-tagged jet, $m(Zb)$, between data and the background prediction in the signal region of the pair-production (PP) $2\ell$ $\geq 2$J channel. The background prediction is shown post-fit, i.e. after the fit to the data $m(Zb)$ distributions under the background-only hypothesis. The last bin contains the overflow. An example distribution for a $B\bar B$ signal in the singlet model with $m_B$ = 900 GeV is overlaid.
A search for heavy resonances decaying into a pair of $Z$ bosons leading to $\ell^+\ell^-\ell'^+\ell'^-$ and $\ell^+\ell^-\nu\bar\nu$ final states, where $\ell$ stands for either an electron or a muon, is presented. The search uses proton-proton collision data at a centre-of-mass energy of 13 TeV collected from 2015 to 2018 that corresponds to the full integrated luminosity of 139 fb$^{-1}$ recorded by the ATLAS detector during Run 2 of the Large Hadron Collider. Different mass ranges spanning 200 GeV to 2000 GeV for the hypothetical resonances are considered, depending on the final state and model. In the absence of a significant observed excess, the results are interpreted as upper limits on the production cross section of a spin-0 or spin-2 resonance. The upper limits for the spin-0 resonance are translated to exclusion contours in the context of Type-I and Type-II two-Higgs-doublet models, and the limits for the spin-2 resonance are used to constrain the Randall--Sundrum model with an extra dimension giving rise to spin-2 graviton excitations.
The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass for the ggF production mode
The upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass for the VBF production mode
The upper limits at 95% CL on the cross section for the ggF production mode times branching ratio as a function of the heavy resonance mass for an additional heavy scalar assuming a width of 1% of its mass
Semi-visible jets, with a significant contribution to the event's missing transverse momentum, can arise in strongly interacting dark sectors. This results in an event topology where one of the jets can be aligned with the direction of the missing transverse momentum. The first search for semi-visible jets produced via a $t$-channel mediator exchange is presented. The analysis uses proton-proton collisions with an integrated luminosity of 139 fb$^{-1}$ and a centre-of-mass energy of 13 TeV, collected with the ATLAS detector during the Run 2 of the LHC. No excess over Standard Model predictions is observed. Assuming a coupling strength of unity between the mediator, a Standard Model quark and a dark quark, mediator masses up to 2.7 TeV are excluded at the 95% confidence level. Upper limits on the coupling strength are also derived.
Observed 95% CL limits on the t-channel production cross-section for semi-visible jets for R$_{inv}$ = 0.1.
Observed 95% CL limits on the t-channel production cross-section for semi-visible jets for R$_{inv}$ = 0.2.
Observed 95% CL limits on the t-channel production cross-section for semi-visible jets for R$_{inv}$ = 0.4.
The results of a search for direct pair production of top squarks and for dark matter in events with two opposite-charge leptons (electrons or muons), jets and missing transverse momentum are reported, using 139 fb$^{-1}$ of integrated luminosity from proton-proton collisions at $\sqrt{s} = 13$ TeV, collected by the ATLAS detector at the Large Hadron Collider during Run 2 (2015-2018). This search considers the pair production of top squarks and is sensitive across a wide range of mass differences between the top squark and the lightest neutralino. Additionally, spin-0 mediator dark-matter models are considered, in which the mediator is produced in association with a pair of top quarks. The mediator subsequently decays to a pair of dark-matter particles. No significant excess of events is observed above the Standard Model background, and limits are set at 95% confidence level. The results exclude top squark masses up to about 1 TeV, and masses of the lightest neutralino up to about 500 GeV. Limits on dark-matter production are set for scalar (pseudoscalar) mediator masses up to about 250 (300) GeV.
Three-body selection. Distributions of $M_{\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the selection criteria of the given SR, except the one for the presented variable, after the background fit. The contributions from all SM backgrounds are shown as a histogram stack. ''Others'' includes contributions from $VVV$, $t\bar{t} t$, $t\bar{t}t\bar{t}$, $t\bar{t} W$, $t\bar{t} WW$, $t\bar{t} WZ$, $t\bar{t} H$, and $tZ$ processes. The hatched bands represent the total statistical and systematic uncertainty. The rightmost bin of each plot includes overflow events. Reference top squark pair production signal models are overlayed for comparison. Red arrows in the upper panels indicate the signal region selection criteria. The bottom panels show the ratio of the observed data to the total SM background prediction, with hatched bands representing the total uncertainty in the background prediction; red arrows show data outside the vertical-axis range.
Three-body selection. Distributions of $M_{\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the selection criteria of the given SR, except the one for the presented variable, after the background fit. The contributions from all SM backgrounds are shown as a histogram stack. ''Others'' includes contributions from $VVV$, $t\bar{t} t$, $t\bar{t}t\bar{t}$, $t\bar{t} W$, $t\bar{t} WW$, $t\bar{t} WZ$, $t\bar{t} H$, and $tZ$ processes. The hatched bands represent the total statistical and systematic uncertainty. The rightmost bin of each plot includes overflow events. Reference top squark pair production signal models are overlayed for comparison. Red arrows in the upper panels indicate the signal region selection criteria. The bottom panels show the ratio of the observed data to the total SM background prediction, with hatched bands representing the total uncertainty in the background prediction; red arrows show data outside the vertical-axis range.
Three-body selection. Distributions of $M_{\Delta}^R$ in (a,b) $SR_{W}^{3-body}$ and (c,d) $SR_{T}^{3-body}$ for (left) same-flavour and (right) different-flavour events satisfying the selection criteria of the given SR, except the one for the presented variable, after the background fit. The contributions from all SM backgrounds are shown as a histogram stack. ''Others'' includes contributions from $VVV$, $t\bar{t} t$, $t\bar{t}t\bar{t}$, $t\bar{t} W$, $t\bar{t} WW$, $t\bar{t} WZ$, $t\bar{t} H$, and $tZ$ processes. The hatched bands represent the total statistical and systematic uncertainty. The rightmost bin of each plot includes overflow events. Reference top squark pair production signal models are overlayed for comparison. Red arrows in the upper panels indicate the signal region selection criteria. The bottom panels show the ratio of the observed data to the total SM background prediction, with hatched bands representing the total uncertainty in the background prediction; red arrows show data outside the vertical-axis range.
A search for the direct production of the supersymmetric partners of $\tau$-leptons (staus) in final states with two hadronically decaying $\tau$-leptons is presented. The analysis uses a dataset of $pp$ collisions corresponding to an integrated luminosity of $139$ fb$^{-1}$, recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of 13 TeV. No significant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of direct production of stau pairs with each stau decaying into the stable lightest neutralino and one $\tau$-lepton in simplified models where the two stau mass eigenstates are degenerate. Stau masses from 120 GeV to 390 GeV are excluded at 95% confidence level for a massless lightest neutralino.
The observed upper limits on the model cross-section in units of pb for simplified models with combined ${\tilde{\tau}}^{+}_{R,L} {\tilde{\tau}}^{-}_{R,L}$ production. Three points at ${M({\tilde{\chi}}^{0}_{1})}=200GeV$ were removed from the plot but kept in the table because they overlapped with the plot's legend and are far from the exclusion contour.
The observed upper limits on the model cross-section in units of pb for simplified models with combined ${\tilde{\tau}}^{+}_{R,L} {\tilde{\tau}}^{-}_{R,L}$ production. Three points at ${M({\tilde{\chi}}^{0}_{1})}=200GeV$ were removed from the plot but kept in the table because they overlapped with the plot's legend and are far from the exclusion contour.
The observed upper limits on the model cross-section in units of pb for simplified models with ${\tilde{\tau}}_L {\tilde{\tau}}_L$ only production. Three points at $M({\tilde{\chi}}^{0}_{1})=200GeV$ were removed from the plot but kept in the table because they overlapped with the plot's legend and are far from the exclusion contour.
A search for a heavy neutral Higgs boson, $A$, decaying into a $Z$ boson and another heavy Higgs boson, $H$, is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC. The search considers the $Z$ boson decaying into electrons or muons and the $H$ boson into a pair of $b$-quarks or $W$ bosons. The mass range considered is 230-800 GeV for the $A$ boson and 130-700 GeV for the $H$ boson. The data are in good agreement with the background predicted by the Standard Model, and therefore 95% confidence-level upper limits for $\sigma \times B(A\rightarrow ZH) \times B(H\rightarrow bb$ or $H\rightarrow WW)$ are set. The upper limits are in the range 0.0062-0.380 pb for the $H\rightarrow bb$ channel and in the range 0.023-8.9 pb for the $H\rightarrow WW$ channel. An interpretation of the results in the context of two-Higgs-Doublet models is also given.
The mass distribution of the bb system before any mbb window cuts for the 2 tag category in b-associated production. The signal distribution for (mA, mH) = (600, 300) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A->ZH)xB(H->bb) corresponds to 1 pb. Background components are displayed separately.
The mass distribution of the bb system before any mbb window cuts for the 3 tag category in b-associated production. The signal distribution for (mA, mH) = (600, 300) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A->ZH)xB(H->bb) corresponds to 1 pb. Background components are displayed separately.
The mllbb mass distribution for the mbb window defined for (mA, mH)=(600, 300) GeV in the 2 tag category with gluon-gluon fusion production is shown. The number of entries shown in each bin is the number of events in that bin divided by the width of the bin. The signal distribution for (mA, mH) = (600, 300) GeV is also shown, and is normalised such that the production cross-section times the branching ratios B(A->ZH)xB(H->bb) corresponds to 1 pb. Background components are displayed separately.
The observation of forward proton scattering in association with lepton pairs ($e^+e^-+p$ or $\mu^+\mu^-+p$) produced via photon fusion is presented. The scattered proton is detected by the ATLAS Forward Proton spectrometer while the leptons are reconstructed by the central ATLAS detector. Proton-proton collision data recorded in 2017 at a center-of-mass energy of $\sqrt{s} = 13$ TeV are analyzed, corresponding to an integrated luminosity of 14.6 fb$^{-1}$. A total of 57 (123) candidates in the $ee+p$ ($\mu\mu+p$) final state are selected, allowing the background-only hypothesis to be rejected with a significance exceeding five standard deviations in each channel. Proton-tagging techniques are introduced for cross-section measurements in the fiducial detector acceptance, corresponding to $\sigma_{ee+p}$ = 11.0 $\pm$ 2.6 (stat.) $\pm$ 1.2 (syst.) $\pm$ 0.3 (lumi.) fb and $\sigma_{\mu\mu+p}$ = 7.2 $\pm$ 1.6 (stat.) $\pm$ 0.9 (syst.) $\pm$ 0.2 (lumi.) fb in the dielectron and dimuon channel, respectively.
The measured fiducial cross sections. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity, the second is the luminosity
This paper reports on a search for the electroweak diboson ($WW/WZ/ZZ$) production in association with a high-mass dijet system, using data from proton-proton collisions at a center-of-mass energy of $\sqrt{s}=13$ TeV. The data, corresponding to an integrated luminosity of 35.5 fb$^{-1}$, were recorded with the ATLAS detector in 2015 and 2016 at the Large Hadron Collider. The search is performed in final states in which one boson decays leptonically, and the other boson decays hadronically. The hadronically decaying $W/Z$ boson is reconstructed as either two small-radius jets or one large-radius jet using jet substructure techniques. The electroweak production of $WW/WZ/ZZ$ in association with two jets is measured with an observed (expected) significance of 2.7 (2.5) standard deviations, and the fiducial cross section is measured to be $45.1 \pm 8.6(\mathrm{stat.}) ^{+15.9} _{-14.6} (\mathrm{syst.})$ fb.
Summary of predicted and measured fiducial cross sections for EW $VVjj$ production. The three lepton channels are combined. For the measured fiducial cross sections in the merged and resolved categories, two signal-strength parameters are used in the combined fit, one for the merged category and the other one for the resolved category; while for the measured fiducial cross section in the inclusive fiducial phase space, a single signal-strength parameter is used. For the SM predicted cross section, the error is the theoretical uncertainty (theo.). For the measured cross section, the first error is the statistical uncertainty (stat.), and the second error is the systematic uncertainty (syst.).
Summary of predicted and measured fiducial cross sections for EW $VVjj$ production. in the three lepton channels. The measured values are obtained from a simultaneous fit where each lepton channel has its own signal-strength parameter, and in each lepton channel the same signal-strength parameter is applied to both the merged and resolved categories. For the SM predicted cross section, the error is the theoretical uncertainty (theo.). For the measured cross section, the first error is the statistical uncertainty (stat.), and the second error is the systematic uncertainty (syst.).
A search is presented for four-top-quark production using an integrated luminosity of 139 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the LHC. Events are selected if they contain a same-sign lepton pair or at least three leptons (electrons or muons). Jet multiplicity, jet flavour and event kinematics are used to separate signal from the background through a multivariate discriminant, and dedicated control regions are used to constrain the dominant backgrounds. The four-top-quark production cross section is measured to be 24$^{+7}_{-6}$ fb. This corresponds to an observed (expected) significance with respect to the background-only hypothesis of 4.3 (2.4) standard deviations and provides evidence for this process.
The results of fitted inclusive ${t\bar{t}t\bar{t}}$ cross-section
The results of the fitted signal strength $\mu$
List of the uncertainties in the signal strength $\mu$, grouped in categories. The quoted values are obtained by repeating the fit, fixing a set of nuisance parameters of the sources corresponding to the considered category, and subtracting in quadrature the resulting uncertainty from the total uncertainty of the nominal fit presented in the last line. The total uncertainty is different from the sum in quadrature of the components due to correlations between nuisance parameters.
A search for new-physics resonances decaying into a lepton and a jet performed by the ATLAS experiment is presented. Scalar leptoquarks pair-produced in $pp$ collisions at $\sqrt{s}=13$ TeV at the Large Hadron Collider are considered using an integrated luminosity of 139 fb$^{-1}$, corresponding to the full Run 2 dataset. They are searched for in events with two electrons or two muons and two or more jets, including jets identified as arising from the fragmentation of $c$- or $b$-quarks. The observed yield in each channel is consistent with the Standard Model background expectation. Leptoquarks with masses below 1.8 TeV and 1.7 TeV are excluded in the electron and muon channels, respectively, assuming a branching ratio into a charged lepton and a quark of 100%, with minimal dependence on the quark flavour. Upper limits on the aforementioned branching ratio are also given as a function of the leptoquark mass.
Distribution of the resonance mass in the pretag Signal Region of the $ qe$ channel for the post-fit background, the observed data, and the expected signal with $m_{LQ} = 1$ TeV.
The observed and expected limits on the leptoquark pair production cross-section at 95% CL for $\mathcal{B}=1$ into electrons, shown as a function of $m_{LQ}$ for the $qe$ channel.
The observed and expected limits on the leptoquark pair production cross-section at 95% CL for $\mathcal{B}=1$ into muons, shown as a function of $m_{LQ}$ for the $q\mu$ channel.
Backward production of ϱ 0 and f 0 mesons in π + n interactions at 6 GeV/ c is presented. Total and differential cross sections are reported along with spin density matrix elements.
This letter presents a search for narrow, high-mass resonances in the $Z\gamma$ final state with the $Z$ boson decaying into a pair of electrons or muons. The $\sqrt{s}=13$ TeV $pp$ collision data were recorded by the ATLAS detector at the CERN Large Hadron Collider and have an integrated luminosity of 140 fb$^{-1}$. The data are found to be in agreement with the Standard Model background expectation. Upper limits are set on the resonance production cross section times the decay branching ratio into $Z\gamma$. For spin-0 resonances produced via gluon-gluon fusion, the observed limits at 95% confidence level vary between 65.5 fb and 0.6 fb, while for spin-2 resonances produced via gluon-gluon fusion (or quark-antiquark initial states) limits vary between 77.4 (76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV to 3400 GeV.
Observed (solid line) and expected (dashed line) 95\% CL limits on the product of the production cross section times the branching ratio of a narrow width spin-0 resonance $X$ produced via gluon-gluon initial states decaying to a $Z$ boson and a photon, $\sigma(pp\to X)\cdot\mathcal{B}(X\to Z\gamma)$, as a function of the resonance mass $m_{X}$. Observed (expected) results are derived from ensemble tests for $m_{X}>1850 (900)$~\GeV. The green and yellow solid bands correspond to the $\pm1\sigma$ and $\pm2\sigma$ intervals for the expected upper limits. The limits in the $m_{X}$ ranges from 220 GeV to 3400 GeV and are obtained from the combined $ee\gamma$ and $\mu\mu\gamma$ channels.
Observed (solid line) and expected (dashed line) 95\% CL limits on the product of the production cross section times the branching ratio of a narrow width spin-2 resonance $X$ produced via gluon-gluon initial states decaying to a $Z$ boson and a photon, $\sigma(pp\to X)\cdot\mathcal{B}(X\to Z\gamma)$, as a function of the resonance mass $m_{X}$. Observed (expected) results are derived from ensemble tests for $m_{X}>1850 (900)$~\GeV. The green and yellow solid bands correspond to the $\pm1\sigma$ and $\pm2\sigma$ intervals for the expected upper limit respectively. The limits in the $m_{X}$ ranges from 220 GeV to 3400 GeV and are obtained from the combined $ee\gamma$ and $\mu\mu\gamma$ channels..
Observed (solid line) and expected (dashed line) 95\% CL limits on the product of the production cross section times the branching ratio of a narrow width spin-2 resonance $X$ produced via $q\bar{q}$ initial states decaying to a $Z$ boson and a photon, $\sigma(pp\to X)\cdot\mathcal{B}(X\to Z\gamma)$, as a function of the resonance mass $m_{X}$. Observed (expected) results are derived from ensemble tests for $m_{X}>1850 (900)$~\GeV. The green and yellow solid bands correspond to the $\pm1\sigma$ and $\pm2\sigma$ intervals for the expected upper limit respectively. The limits in the $m_{X}$ ranges from 220 GeV to 3400 GeV and are obtained from the combined $ee\gamma$ and $\mu\mu\gamma$ channels.
This paper reports cross-section measurements of $ZZ$ production in $pp$ collisions at $\sqrt{s}=13.6$ TeV at the Large Hadron Collider. The data were collected by the ATLAS detector in 2022, and correspond to an integrated luminosity of 29 fb$^-1$. Events in the $ZZ\rightarrow4\ell$ ($\ell = e$, $\mu$) final states are selected and used to measure the inclusive and differential cross-sections in a fiducial region defined close to the analysis selections. The inclusive cross-section is further extrapolated to the total phase space with a requirement of 66 $< m_Z <$ 116 GeV for both $Z$ bosons, yielding $16.8 \pm 1.1$ pb. The results are well described by the Standard Model predictions.
The measured differential cross-sections compared to the predictions in the $m_{4\ell}$ bins
The measured differential cross-sections compared to the predictions in the $p_T^{4\ell}$ bins
The $t\bar{t}$ production cross-section is measured in the lepton+jets channel using proton$-$proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected with the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 139 fb$^{-1}$. Events with exactly one charged lepton and four or more jets in the final state, with at least one jet containing $b$-hadrons, are used to determine the $t\bar{t}$ production cross-section through a profile-likelihood fit. The inclusive cross-section is measured to be ${\sigma_{\text{inc}} = 830 \pm 0.4~ \text{(stat.)}\pm 36~\text{(syst.)}\pm 14~\text{(lumi.)}~\mathrm{pb}}$ with a relative uncertainty of 4.6 %. The result is consistent with theoretical calculations at next-to-next-to-leading order in perturbative QCD. The fiducial $t\bar{t}$ cross-section within the experimental acceptance is also measured.
The results of fitted inclusive and fiducial ${t\bar{t}}$ cross-sections
The results of fitted inclusive and fiducial ${t\bar{t}}$ cross-sections
Ranking of the systematic uncertainties on the measured cross-section, normalised to the predicted value, in the inclusive fit to data. The impact of each nuisance parameter, $\Delta \sigma_{\text{inc}}/\sigma^{\text{pred.}}_{\text{inc}}$, is computed by comparing the nominal best-fit value of $\sigma_{\text{inc}}/\sigma^{\text{pred}}_{\text{inc}}$ with the result of the fit when fixing the considered nuisance parameter to its best-fit value, $\theta$, shifted by its pre-fit (post-fit) uncertainties $\pm \Delta \theta$ ($\pm \Delta \hat{\theta}$). The figure shows the effect of the ten most significant uncertainties.
This paper presents a search for new heavy particles decaying into a pair of top quarks using 139 fb$^{-1}$ of proton--proton collision data recorded at a centre-of-mass energy of $\sqrt{s}=13$ TeV with the ATLAS detector at the Large Hadron Collider. The search is performed using events consistent with pair production of high-transverse-momentum top quarks and their subsequent decays into the fully hadronic final states. The analysis is optimized for resonances decaying into a $t\bar{t}$ pair with mass above 1.4 TeV, exploiting a dedicated multivariate technique with jet substructure to identify hadronically decaying top quarks using large-radius jets and evaluating the background expectation from data. No significant deviation from the background prediction is observed. Limits are set on the production cross-section times branching fraction for the new $Z'$ boson in a topcolor-assisted-technicolor model. The $Z'$ boson masses below 3.9 and 4.7 TeV are excluded at 95% confidence level for the decay widths of 1% and 3%, respectively.
Acceptance and acceptance times selection efficiency as a function of $m^{gen}_{t\bar{t}}$ in SR$1b$. The acceptance is measured as the fraction of events with two leading truth-contained large-$R$ jets, both satisfying the kinematic requirements, but not containing generator-level electrons or muons, as described in the paper. The acceptance $\times$ efficiency is calculated with respect to the full analysis selections including top- and $b$-tagging requirements on the two leading large-$R$ jets. The $m^{gen}_{t\bar{t}}$ is calculated from the momenta of top and anti-top quarks at the generator level before final-state radiation. The branching fractions of the $t \bar{t}$ into all possible final states are included in the acceptance calculation.
Acceptance and acceptance times selection efficiency as a function of $m^{gen}_{t\bar{t}}$ in SR$2b$. The acceptance is measured as the fraction of events with two leading truth-contained large-$R$ jets, both satisfying the kinematic requirements, but not containing generator-level electrons or muons, as described in the paper. The acceptance $\times$ efficiency is calculated with respect to the full analysis selections including top- and $b$-tagging requirements on the two leading large-$R$ jets. The $m^{gen}_{t\bar{t}}$ is calculated from the momenta of top and anti-top quarks at the generator level before final-state radiation. The branching fractions of the $t \bar{t}$ into all possible final states are included in the acceptance calculation.
Observed $m_{t\bar{t}}^{reco}$ distributions in data for SR$1b$, shown together with the result of the fit with the three-shape-parameter function. The error bars indicate the effect of the fit parameter uncertainty on the background prediction. The bin width of the distributions is chosen to be the same as that used in the background parameterization.
The production of a $W$ boson in association with a single charm quark is studied using 140 $\mathrm{fb}^{-1}$ of $\sqrt{s} = 13\,\mathrm{TeV}$ proton-proton collision data collected with the ATLAS detector at the Large Hadron Collider. The charm quark is tagged by a charmed hadron, reconstructed with a secondary-vertex fit. The $W$ boson is reconstructed from an electron/muon decay and the missing transverse momentum. The mesons reconstructed are $D^{\pm} \to K^\mp \pi^\pm \pi^\pm$ and $D^{*\pm} \to D^{0} \pi^\pm \to (K^\mp \pi^\pm) \pi^\pm$, where $p_{\text{T}}(e, \mu) > 30\,\mathrm{GeV}$, $|\eta(e, \mu)| < 2.5$, $p_{\text{T}}(D) > 8\,\mathrm{GeV}$, and $|\eta(D)| < 2.2$. The integrated and normalized differential cross-sections as a function of the pseudorapidity of the lepton from the $W$ boson decay, and of the transverse momentum of the meson, are extracted from the data using a profile likelihood fit. The measured fiducial cross-sections are $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{-}{+}D^{+}) = 50.2\pm0.2\,\mathrm{(stat.)}\,^{+2.4}_{-2.3}\,\mathrm{(syst.)}\,\mathrm{pb}$, $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{+}{+}D^{-}) = 48.5\pm0.2\,\mathrm{(stat.)}\,^{+2.3}_{-2.2}\,\mathrm{(syst.)}\,\mathrm{pb}$, $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{-}{+}D^{*+}) = 51.1\pm0.4\,\mathrm{(stat.)}\,^{+1.9}_{-1.8}\,\mathrm{(syst.)}\,\mathrm{pb}$, and $\sigma^{\mathrm{OS-SS}}_{\mathrm{fid}}(W^{+}{+}D^{*-}) = 50.0\pm0.4\,\mathrm{(stat.)}\,^{+1.9}_{-1.8}\,\mathrm{(syst.)}\,\mathrm{pb}$. Results are compared with the predictions of next-to-leading-order quantum chromodynamics calculations performed using state-of-the-art parton distribution functions. The ratio of charm to anti-charm production cross-sections is studied to probe the $s$-$\bar{s}$ quark asymmetry and is found to be $R_c^\pm = 0.971\pm0.006\,\mathrm{(stat.)}\pm0.011\,\mathrm{(syst.)}$.
Measured fiducial cross-sections times the single-lepton-flavor W boson branching ratio.
Measured cross section ratios for the W+D production. The $R_{c}(D^{(*)})$ observable is obtained by combining the individual measurements of $R_{c}(D^{+})$ and $R_{c}(D^{*+})$ as explained in the text. The displayed cross sections are integrated over each differential bin.
Measured $p_{\mathrm{T}}(D^{+})$ differential fiducial cross-section times the single-lepton-flavor W boson branching ratio in the $W^{-}+D^{+}$ channel. The last $p_{\mathrm{T}}$ bin has no upper bound. The displayed cross sections are integrated over each differential bin.
None
FIRST CROSS SECTION GIVEN WITH MORE DETAILS IN S. TOAFF ET AL., NP B146, 368 (1978). THE SECOND CROSS SECTION IS CALCULATED FROM THE FIRST USING ISOSPIN SYMMETRY.
This paper reports on a search for heavy resonances decaying into $WW$, $ZZ$ or $WZ$ using proton-proton collision data at a centre-of-mass energy of $\sqrt{s}=13$ TeV. The data, corresponding to an integrated luminosity of 139 $\mathrm{fb^{-1}}$, were recorded with the ATLAS detector from 2015 to 2018 at the Large Hadron Collider. The search is performed for final states in which one $W$ or $Z$ boson decays leptonically, and the other $W$ boson or $Z$ boson decays hadronically. The data are found to be described well by expected backgrounds. Upper bounds on the production cross sections of heavy scalar, vector or tensor resonances are derived in the mass range 300-5000 GeV within the context of Standard Model extensions with warped extra dimensions or including a heavy vector triplet. Production through gluon-gluon fusion, Drell-Yan or vector-boson fusion are considered, depending on the assumed model.
Selection acceptance times efficiency for the 0 leptons signal events from MC simulations as a function of the resonance mass for ggF/DY production.
Selection acceptance times efficiency for the 0 leptons signal events from MC simulations as a function of the resonance mass for VBF production.
Selection acceptance times efficiency for the 1 lepton signal events from MC simulations as a function of the resonance mass for ggF/DY production.
A search for supersymmetry through the pair production of electroweakinos with mass splittings near the electroweak scale and decaying via on-shell $W$ and $Z$ bosons is presented for a three-lepton final state. The analyzed proton-proton collision data taken at a center-of-mass energy of $\sqrt{s}$ = 13 TeV were collected between 2015 and 2018 by the ATLAS experiment at the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. A search, emulating the recursive jigsaw reconstruction technique with easily reproducible laboratory-frame variables, is performed. The two excesses observed in the 2015-2016 data recursive jigsaw analysis in the low-mass three-lepton phase space are reproduced. Results with the full dataset are in agreement with the Standard Model expectations. They are interpreted to set exclusion limits at 95% confidence level on simplified models of chargino-neutralino pair production for masses up to 345 GeV.
Distributions in SR-low of the data and post-fit background prediction for m<sub>T</sub>. The SR-low event selections are applied for each distribution except for the variable shown, where the selection is indicated by a red arrow. The normalization factor for the WZ background is derived from the background-only estimation described in Section 7. The expected distribution for a benchmark signal model is included for comparison. The first (last) bin includes underflow (overflow). The "Top-quark like" category contains the tt̄, Wt, and WW processes while the "Others" category contains backgrounds from triboson production and processes that include a Higgs boson, 3 or more tops, and tops produced in association with W or Z bosons. The bottom panel shows the ratio of the data to the post-fit background prediction. The hatched bands indicate the combined theoretical, experimental, and MC statistical uncertainties.
Distributions in SR-low of the data and post-fit background prediction for m<sub>T</sub>. The SR-low event selections are applied for each distribution except for the variable shown, where the selection is indicated by a red arrow. The normalization factor for the WZ background is derived from the background-only estimation described in Section 7. The expected distribution for a benchmark signal model is included for comparison. The first (last) bin includes underflow (overflow). The "Top-quark like" category contains the tt̄, Wt, and WW processes while the "Others" category contains backgrounds from triboson production and processes that include a Higgs boson, 3 or more tops, and tops produced in association with W or Z bosons. The bottom panel shows the ratio of the data to the post-fit background prediction. The hatched bands indicate the combined theoretical, experimental, and MC statistical uncertainties.
Distributions in SR-low of the data and post-fit background prediction for H<sup>boost</sup>. The SR-low event selections are applied for each distribution except for the variable shown, where the selection is indicated by a red arrow. The normalization factor for the WZ background is derived from the background-only estimation described in Section 7. The expected distribution for a benchmark signal model is included for comparison. The first (last) bin includes underflow (overflow). The "Top-quark like" category contains the tt̄, Wt, and WW processes while the "Others" category contains backgrounds from triboson production and processes that include a Higgs boson, 3 or more tops, and tops produced in association with W or Z bosons. The bottom panel shows the ratio of the data to the post-fit background prediction. The hatched bands indicate the combined theoretical, experimental, and MC statistical uncertainties.
The results of a search for electroweakino pair production $pp \rightarrow \tilde\chi^\pm_1 \tilde\chi^0_2$ in which the chargino ($\tilde\chi^\pm_1$) decays into a $W$ boson and the lightest neutralino ($\tilde\chi^0_1$), while the heavier neutralino ($\tilde\chi^0_2$) decays into the Standard Model 125 GeV Higgs boson and a second $\tilde\chi^0_1$ are presented. The signal selection requires a pair of $b$-tagged jets consistent with those from a Higgs boson decay, and either an electron or a muon from the $W$ boson decay, together with missing transverse momentum from the corresponding neutrino and the stable neutralinos. The analysis is based on data corresponding to 139 $\mathrm{fb}^{-1}$ of $\sqrt{s}=13$ TeV $pp$ collisions provided by the Large Hadron Collider and recorded by the ATLAS detector. No statistically significant evidence of an excess of events above the Standard Model expectation is found. Limits are set on the direct production of the electroweakinos in simplified models, assuming pure wino cross-sections. Masses of $\tilde{\chi}^{\pm}_{1}/\tilde{\chi}^{0}_{2}$ up to 740 GeV are excluded at 95% confidence level for a massless $\tilde{\chi}^{0}_{1}$.
The observed exclusion for simplified models with $\tilde\chi^\pm_1 \tilde\chi^0_2 \rightarrow Wh\tilde\chi^0_1\tilde\chi^0_1, W \rightarrow l\nu, h \rightarrow b\bar{b}$ production. Experimental and theoretical systematic uncertainties are applied to background and signal samples and illustrated by the yellow band and the red dotted contour lines, respectively. The red dotted lines indicate the $\pm$ 1 standard-deviation variation on the observed exclusion limit due to theoretical uncertainties in the signal cross-section.
The observed exclusion for simplified models with $\tilde\chi^\pm_1 \tilde\chi^0_2 \rightarrow Wh\tilde\chi^0_1\tilde\chi^0_1, W \rightarrow l\nu, h \rightarrow b\bar{b}$ production. Experimental and theoretical systematic uncertainties are applied to background and signal samples and illustrated by the yellow band and the red dotted contour lines, respectively. The red dotted lines indicate the $\pm$ 1 standard-deviation variation on the observed exclusion limit due to theoretical uncertainties in the signal cross-section.
The observed exclusion for simplified models with $\tilde\chi^\pm_1 \tilde\chi^0_2 \rightarrow Wh\tilde\chi^0_1\tilde\chi^0_1, W \rightarrow l\nu, h \rightarrow b\bar{b}$ production. Experimental and theoretical systematic uncertainties are applied to background and signal samples and illustrated by the yellow band and the red dotted contour lines, respectively. The red dotted lines indicate the $\pm$ 1 standard-deviation variation on the observed exclusion limit due to theoretical uncertainties in the signal cross-section.
A search for magnetic monopoles and high-electric-charge objects is presented using 34.4 fb$^{-1}$ of 13 TeV $pp$ collision data collected by the ATLAS detector at the LHC during 2015 and 2016. The considered signature is based upon high ionization in the transition radiation tracker of the inner detector associated with a pencil-shape energy deposit in the electromagnetic calorimeter. The data were collected by a dedicated trigger based on the tracker high-threshold hit capability. The results are interpreted in models of Drell-Yan pair production of stable particles with two spin hypotheses (0 and 1/2) and masses ranging from 200 GeV to 4000 GeV. The search improves by approximately a factor of five the constraints on the direct production of magnetic monopoles carrying one or two Dirac magnetic charges and stable objects with electric charge in the range $20\le|z|\le60$ and extends the charge range to $60<|z|\le100$.
Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-0 monopole production as a function of mass for magnetic charges $|g|=1g_D$ and $|g|=2g_D$.
Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-0 HECO production as a function of mass for various values of electric charge in the range $20\le|z|\le100$.
Observed 95% confidence-level upper limits on the cross section for Drell-Yan spin-1/2 monopole production as a function of mass for magnetic charges $|g|=1g_D$ and $|g|=2g_D$.
Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\mathrm{fb}^{-1}$. Due to the large $t\bar{t}$ cross-section at the LHC, such measurements allow a detailed study of the properties of top-quark production and decay, enabling precision tests of several Monte Carlo generators and fixed-order Standard Model predictions. Overall, there is good agreement between the theoretical predictions and the data.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definitions:</b><br/> <i>Resolved:</i> <ul> <li> NLEP = 1, either E or MU, PT > 27 GeV, ABS ETA < 2.5 <li> NJETS >= 4, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 2 </ul><br/> <i>Boosted:</i> <ul> <li> NLEP = 1, either E or MU, PT > 27 GeV, ABS ETA < 2.5 <li> NJETS >= 1, R = 0.4, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 1 <li> NJETS >= 1, R=1, PT > 350 GeV, ABS ETA < 2.0, top-tagged </ul><br/> <b>Particle level:</b><br/> <i>Resolved:</i><br/> <u>1D:</u><br/> Spectra: <ul> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1">Table 1</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 3">Table 3</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 5">Table 5</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 7">Table 7</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 9">Table 9</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 11">Table 11</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 13">Table 13</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 15">Table 15</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 17">Table 17</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 19">Table 19</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 21">Table 21</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 23">Table 23</a> ) <li>1/SIG*DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 25">Table 25</a> ) <li>DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 27">Table 27</a> ) <li>1/SIG*DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 29">Table 29</a> ) <li>DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 31">Table 31</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 33">Table 33</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 35">Table 35</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 37">Table 37</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 39">Table 39</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 41">Table 41</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 43">Table 43</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 45">Table 45</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 47">Table 47</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 49">Table 49</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 51">Table 51</a> ) <li>SIG (<a href="95758?version=1&table=Table 53">Table 53</a> ) </ul><br/> Covariances: <ul> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 2">Table 2</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 4">Table 4</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 6">Table 6</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 8">Table 8</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 10">Table 10</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 12">Table 12</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 14">Table 14</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 16">Table 16</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 18">Table 18</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 20">Table 20</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 22">Table 22</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 24">Table 24</a> ) <li>1/SIG*DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 26">Table 26</a> ) <li>DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 28">Table 28</a> ) <li>1/SIG*DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 30">Table 30</a> ) <li>DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 32">Table 32</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 34">Table 34</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 36">Table 36</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 38">Table 38</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 40">Table 40</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 42">Table 42</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 44">Table 44</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 46">Table 46</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 48">Table 48</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 50">Table 50</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 52">Table 52</a> ) </ul><br/> Inter-spectra correlations: <ul> <li>Statistical correlation between DSIG/DPT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 518">Table 518</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 519">Table 519</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 520">Table 520</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 521">Table 521</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 522">Table 522</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 523">Table 523</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 524">Table 524</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 525">Table 525</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 526">Table 526</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 527">Table 527</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 528">Table 528</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 529">Table 529</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 530">Table 530</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 531">Table 531</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 532">Table 532</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 533">Table 533</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 534">Table 534</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 535">Table 535</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 536">Table 536</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 537">Table 537</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 538">Table 538</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 539">Table 539</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 540">Table 540</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 541">Table 541</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 542">Table 542</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 543">Table 543</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 544">Table 544</a> ) <li>Statistical correlation between DSIG/DABS_POUT_THAD and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 545">Table 545</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 546">Table 546</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 547">Table 547</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 548">Table 548</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 549">Table 549</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 550">Table 550</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 551">Table 551</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 552">Table 552</a> ) <li>Statistical correlation between DSIG/DDPHI_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 553">Table 553</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 554">Table 554</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 555">Table 555</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 556">Table 556</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 557">Table 557</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 558">Table 558</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 559">Table 559</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 560">Table 560</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 561">Table 561</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 562">Table 562</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 563">Table 563</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 564">Table 564</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 565">Table 565</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 566">Table 566</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 567">Table 567</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 568">Table 568</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 569">Table 569</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 570">Table 570</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 571">Table 571</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 572">Table 572</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 573">Table 573</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 574">Table 574</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 575">Table 575</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 576">Table 576</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 577">Table 577</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 578">Table 578</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 579">Table 579</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 580">Table 580</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 581">Table 581</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 582">Table 582</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 583">Table 583</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 584">Table 584</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 585">Table 585</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 586">Table 586</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 587">Table 587</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 588">Table 588</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 589">Table 589</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 590">Table 590</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 591">Table 591</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 592">Table 592</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 593">Table 593</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 594">Table 594</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 595">Table 595</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 596">Table 596</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 597">Table 597</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 598">Table 598</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 599">Table 599</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 600">Table 600</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 601">Table 601</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_POUT_THAD (<a href="95758?version=1&table=Table 602">Table 602</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DDPHI_TTBAR (<a href="95758?version=1&table=Table 603">Table 603</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 604">Table 604</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 605">Table 605</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 606">Table 606</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 607">Table 607</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 608">Table 608</a> ) </ul><br/> <u>2D:</u><br/> Spectra: <ul> <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 54">Table 54</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 55">Table 55</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 56">Table 56</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 57">Table 57</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 58">Table 58</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 74">Table 74</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 75">Table 75</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 76">Table 76</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 77">Table 77</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 78">Table 78</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 94">Table 94</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 95">Table 95</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 96">Table 96</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 97">Table 97</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 98">Table 98</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 200.0 GeV < M_TTBAR < 400.0 GeV) (<a href="95758?version=1&table=Table 114">Table 114</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 400.0 GeV < M_TTBAR < 550.0 GeV) (<a href="95758?version=1&table=Table 115">Table 115</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 550.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 116">Table 116</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 117">Table 117</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 118">Table 118</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 0.0 GeV < PT_THAD < 60.0 GeV) (<a href="95758?version=1&table=Table 134">Table 134</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 60.0 GeV < PT_THAD < 120.0 GeV) (<a href="95758?version=1&table=Table 135">Table 135</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 120.0 GeV < PT_THAD < 200.0 GeV) (<a href="95758?version=1&table=Table 136">Table 136</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 200.0 GeV < PT_THAD < 300.0 GeV) (<a href="95758?version=1&table=Table 137">Table 137</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD ( 300.0 GeV < PT_THAD < 1000.0 GeV) (<a href="95758?version=1&table=Table 138">Table 138</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 0.0 GeV < PT_THAD < 60.0 GeV) (<a href="95758?version=1&table=Table 154">Table 154</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 60.0 GeV < PT_THAD < 120.0 GeV) (<a href="95758?version=1&table=Table 155">Table 155</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 120.0 GeV < PT_THAD < 200.0 GeV) (<a href="95758?version=1&table=Table 156">Table 156</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 200.0 GeV < PT_THAD < 300.0 GeV) (<a href="95758?version=1&table=Table 157">Table 157</a> ) <li>D2SIG/DABS_POUT_THAD/DPT_THAD ( 300.0 GeV < PT_THAD < 1000.0 GeV) (<a href="95758?version=1&table=Table 158">Table 158</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 174">Table 174</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 175">Table 175</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 176">Table 176</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 177">Table 177</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 188">Table 188</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 189">Table 189</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 190">Table 190</a> ) <li>D2SIG/DPT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 191">Table 191</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 202">Table 202</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 203">Table 203</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_JETS (N_JETS $\geq$ 6.0) (<a href="95758?version=1&table=Table 204">Table 204</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 211">Table 211</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 212">Table 212</a> ) <li>D2SIG/DM_TTBAR/DN_JETS (N_JETS $\geq$ 6.0) (<a href="95758?version=1&table=Table 213">Table 213</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 220">Table 220</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 221">Table 221</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 222">Table 222</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 223">Table 223</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 234">Table 234</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 235">Table 235</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 236">Table 236</a> ) <li>D2SIG/DPT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 237">Table 237</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 248">Table 248</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 249">Table 249</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 250">Table 250</a> ) <li>1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 251">Table 251</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 262">Table 262</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 263">Table 263</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 264">Table 264</a> ) <li>D2SIG/DABS_POUT_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 265">Table 265</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 3.5 < N_JETS < 4.5 ) (<a href="95758?version=1&table=Table 276">Table 276</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 4.5 < N_JETS < 5.5 ) (<a href="95758?version=1&table=Table 277">Table 277</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 5.5 < N_JETS < 6.5 ) (<a href="95758?version=1&table=Table 278">Table 278</a> ) <li>1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS ( 6.5 < N_JETS < 7.5 ) (<a href="95758?version=1&table=Table 279">Table 279</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 3.5 < N_JETS < 4.5 ) (<a href="95758?version=1&table=Table 290">Table 290</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 4.5 < N_JETS < 5.5 ) (<a href="95758?version=1&table=Table 291">Table 291</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 5.5 < N_JETS < 6.5 ) (<a href="95758?version=1&table=Table 292">Table 292</a> ) <li>D2SIG/DDPHI_TTBAR/DN_JETS ( 6.5 < N_JETS < 7.5 ) (<a href="95758?version=1&table=Table 293">Table 293</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 304">Table 304</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 305">Table 305</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 306">Table 306</a> ) <li>1/SIG*D2SIG/DHT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 307">Table 307</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 318">Table 318</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 319">Table 319</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 320">Table 320</a> ) <li>D2SIG/DHT_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 321">Table 321</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 332">Table 332</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 333">Table 333</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 334">Table 334</a> ) <li>1/SIG*D2SIG/DABS_Y_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 335">Table 335</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 346">Table 346</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 347">Table 347</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 348">Table 348</a> ) <li>D2SIG/DABS_Y_THAD/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 349">Table 349</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 360">Table 360</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 361">Table 361</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 362">Table 362</a> ) <li>1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 363">Table 363</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 374">Table 374</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 375">Table 375</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 376">Table 376</a> ) <li>D2SIG/DABS_Y_TTBAR/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 377">Table 377</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 388">Table 388</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 389">Table 389</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 390">Table 390</a> ) <li>1/SIG*D2SIG/DCHI_TT/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 391">Table 391</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 4.0) (<a href="95758?version=1&table=Table 402">Table 402</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 5.0) (<a href="95758?version=1&table=Table 403">Table 403</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS = 6.0) (<a href="95758?version=1&table=Table 404">Table 404</a> ) <li>D2SIG/DCHI_TT/DN_JETS (N_JETS $\geq$ 7.0) (<a href="95758?version=1&table=Table 405">Table 405</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 0.7 ) (<a href="95758?version=1&table=Table 416">Table 416</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.7 < ABS_Y_THAD < 1.4 ) (<a href="95758?version=1&table=Table 417">Table 417</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 1.4 < ABS_Y_THAD < 2.5 ) (<a href="95758?version=1&table=Table 418">Table 418</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 0.7 ) (<a href="95758?version=1&table=Table 425">Table 425</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.7 < ABS_Y_THAD < 1.4 ) (<a href="95758?version=1&table=Table 426">Table 426</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 1.4 < ABS_Y_THAD < 2.5 ) (<a href="95758?version=1&table=Table 427">Table 427</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 434">Table 434</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 435">Table 435</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 436">Table 436</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 437">Table 437</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 448">Table 448</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 449">Table 449</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 450">Table 450</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 451">Table 451</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 462">Table 462</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 463">Table 463</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 464">Table 464</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 465">Table 465</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.4 ) (<a href="95758?version=1&table=Table 476">Table 476</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.4 < ABS_Y_TTBAR < 0.8 ) (<a href="95758?version=1&table=Table 477">Table 477</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.8 < ABS_Y_TTBAR < 1.2 ) (<a href="95758?version=1&table=Table 478">Table 478</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.2 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 479">Table 479</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 30.0 GeV) (<a href="95758?version=1&table=Table 490">Table 490</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 30.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 491">Table 491</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 190.0 GeV) (<a href="95758?version=1&table=Table 492">Table 492</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 190.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 493">Table 493</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 30.0 GeV) (<a href="95758?version=1&table=Table 504">Table 504</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 30.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 505">Table 505</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 190.0 GeV) (<a href="95758?version=1&table=Table 506">Table 506</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 190.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 507">Table 507</a> ) </ul><br/> Covariances:<br/><ul> <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 59">Table 59</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 60">Table 60</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 61">Table 61</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 62">Table 62</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 63">Table 63</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 64">Table 64</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 65">Table 65</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 66">Table 66</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 67">Table 67</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 68">Table 68</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 69">Table 69</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 70">Table 70</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 71">Table 71</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 72">Table 72</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 73">Table 73</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 79">Table 79</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 80">Table 80</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 81">Table 81</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 82">Table 82</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 83">Table 83</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 84">Table 84</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 85">Table 85</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 86">Table 86</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 87">Table 87</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 88">Table 88</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 89">Table 89</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 90">Table 90</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 91">Table 91</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 92">Table 92</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 93">Table 93</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 99">Table 99</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 100">Table 100</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 101">Table 101</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 102">Table 102</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 103">Table 103</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 104">Table 104</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 105">Table 105</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 106">Table 106</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 107">Table 107</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 108">Table 108</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 109">Table 109</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 110">Table 110</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 111">Table 111</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 112">Table 112</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 113">Table 113</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 119">Table 119</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 120">Table 120</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 121">Table 121</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 122">Table 122</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 123">Table 123</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 124">Table 124</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 125">Table 125</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 126">Table 126</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 127">Table 127</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 128">Table 128</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 129">Table 129</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 130">Table 130</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 131">Table 131</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 132">Table 132</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 5th and 5th bins of M_TTBAR (<a href="95758?version=1&table=Table 133">Table 133</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 1th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 139">Table 139</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 140">Table 140</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 141">Table 141</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 142">Table 142</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 143">Table 143</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 144">Table 144</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 145">Table 145</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 146">Table 146</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 147">Table 147</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 148">Table 148</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 149">Table 149</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 150">Table 150</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 151">Table 151</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 152">Table 152</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 5th bins of PT_THAD (<a href="95758?version=1&table=Table 153">Table 153</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 1th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 159">Table 159</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 160">Table 160</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 2th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 161">Table 161</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 162">Table 162</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 163">Table 163</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 3th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 164">Table 164</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 165">Table 165</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 166">Table 166</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 167">Table 167</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 4th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 168">Table 168</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 1th bins of PT_THAD (<a href="95758?version=1&table=Table 169">Table 169</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 2th bins of PT_THAD (<a href="95758?version=1&table=Table 170">Table 170</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 3th bins of PT_THAD (<a href="95758?version=1&table=Table 171">Table 171</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 4th bins of PT_THAD (<a href="95758?version=1&table=Table 172">Table 172</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DPT_THAD between the 5th and 5th bins of PT_THAD (<a href="95758?version=1&table=Table 173">Table 173</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 178">Table 178</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 179">Table 179</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 180">Table 180</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 181">Table 181</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 182">Table 182</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 183">Table 183</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 184">Table 184</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 185">Table 185</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 186">Table 186</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 187">Table 187</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 192">Table 192</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 193">Table 193</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 194">Table 194</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 195">Table 195</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 196">Table 196</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 197">Table 197</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 198">Table 198</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 199">Table 199</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 200">Table 200</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 201">Table 201</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 205">Table 205</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 206">Table 206</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 207">Table 207</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 208">Table 208</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 209">Table 209</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 210">Table 210</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 214">Table 214</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 215">Table 215</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 216">Table 216</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 217">Table 217</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 218">Table 218</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 219">Table 219</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 224">Table 224</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 225">Table 225</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 226">Table 226</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 227">Table 227</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 228">Table 228</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 229">Table 229</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 230">Table 230</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 231">Table 231</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 232">Table 232</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 233">Table 233</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 238">Table 238</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 239">Table 239</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 240">Table 240</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 241">Table 241</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 242">Table 242</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 243">Table 243</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 244">Table 244</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 245">Table 245</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 246">Table 246</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 247">Table 247</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 252">Table 252</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 253">Table 253</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 254">Table 254</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 255">Table 255</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 256">Table 256</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 257">Table 257</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 258">Table 258</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 259">Table 259</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 260">Table 260</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 261">Table 261</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 266">Table 266</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 267">Table 267</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 268">Table 268</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 269">Table 269</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 270">Table 270</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 271">Table 271</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 272">Table 272</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 273">Table 273</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 274">Table 274</a> ) <li>Matrix for D2SIG/DABS_POUT_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 275">Table 275</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 280">Table 280</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 281">Table 281</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 282">Table 282</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 283">Table 283</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 284">Table 284</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 285">Table 285</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 286">Table 286</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 287">Table 287</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 288">Table 288</a> ) <li>Matrix for 1/SIG*D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 289">Table 289</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 294">Table 294</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 295">Table 295</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 296">Table 296</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 297">Table 297</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 298">Table 298</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 299">Table 299</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 300">Table 300</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 301">Table 301</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 302">Table 302</a> ) <li>Matrix for D2SIG/DDPHI_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 303">Table 303</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 308">Table 308</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 309">Table 309</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 310">Table 310</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 311">Table 311</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 312">Table 312</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 313">Table 313</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 314">Table 314</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 315">Table 315</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 316">Table 316</a> ) <li>Matrix for 1/SIG*D2SIG/DHT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 317">Table 317</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 322">Table 322</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 323">Table 323</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 324">Table 324</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 325">Table 325</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 326">Table 326</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 327">Table 327</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 328">Table 328</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 329">Table 329</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 330">Table 330</a> ) <li>Matrix for D2SIG/DHT_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 331">Table 331</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 336">Table 336</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 337">Table 337</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 338">Table 338</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 339">Table 339</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 340">Table 340</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 341">Table 341</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 342">Table 342</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 343">Table 343</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 344">Table 344</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 345">Table 345</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 350">Table 350</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 351">Table 351</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 352">Table 352</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 353">Table 353</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 354">Table 354</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 355">Table 355</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 356">Table 356</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 357">Table 357</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 358">Table 358</a> ) <li>Matrix for D2SIG/DABS_Y_THAD/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 359">Table 359</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 364">Table 364</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 365">Table 365</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 366">Table 366</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 367">Table 367</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 368">Table 368</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 369">Table 369</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 370">Table 370</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 371">Table 371</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 372">Table 372</a> ) <li>Matrix for 1/SIG*D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 373">Table 373</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 378">Table 378</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 379">Table 379</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 380">Table 380</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 381">Table 381</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 382">Table 382</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 383">Table 383</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 384">Table 384</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 385">Table 385</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 386">Table 386</a> ) <li>Matrix for D2SIG/DABS_Y_TTBAR/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 387">Table 387</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 392">Table 392</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 393">Table 393</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 394">Table 394</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 395">Table 395</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 396">Table 396</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 397">Table 397</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 398">Table 398</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 399">Table 399</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 400">Table 400</a> ) <li>Matrix for 1/SIG*D2SIG/DCHI_TT/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 401">Table 401</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 1th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 406">Table 406</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 2th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 407">Table 407</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 2th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 408">Table 408</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 409">Table 409</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 410">Table 410</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 3th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 411">Table 411</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 1th bins of N_JETS (<a href="95758?version=1&table=Table 412">Table 412</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 2th bins of N_JETS (<a href="95758?version=1&table=Table 413">Table 413</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 3th bins of N_JETS (<a href="95758?version=1&table=Table 414">Table 414</a> ) <li>Matrix for D2SIG/DCHI_TT/DN_JETS between the 4th and 4th bins of N_JETS (<a href="95758?version=1&table=Table 415">Table 415</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 419">Table 419</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 420">Table 420</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 421">Table 421</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 422">Table 422</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 423">Table 423</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 3th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 424">Table 424</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 428">Table 428</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 429">Table 429</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 430">Table 430</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 431">Table 431</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 432">Table 432</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 3th and 3th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 433">Table 433</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 438">Table 438</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 439">Table 439</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 440">Table 440</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 441">Table 441</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 442">Table 442</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 443">Table 443</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 444">Table 444</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 445">Table 445</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 446">Table 446</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 447">Table 447</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 452">Table 452</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 453">Table 453</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 454">Table 454</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 455">Table 455</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 456">Table 456</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 457">Table 457</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 458">Table 458</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 459">Table 459</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 460">Table 460</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 461">Table 461</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 466">Table 466</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 467">Table 467</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 468">Table 468</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 469">Table 469</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 470">Table 470</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 471">Table 471</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 472">Table 472</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 473">Table 473</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 474">Table 474</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 475">Table 475</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 480">Table 480</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 481">Table 481</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 482">Table 482</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 483">Table 483</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 484">Table 484</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 485">Table 485</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 486">Table 486</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 487">Table 487</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 488">Table 488</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 489">Table 489</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 494">Table 494</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 495">Table 495</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 496">Table 496</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 497">Table 497</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 498">Table 498</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 499">Table 499</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 500">Table 500</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 501">Table 501</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 502">Table 502</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 503">Table 503</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 508">Table 508</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 509">Table 509</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 510">Table 510</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 511">Table 511</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 512">Table 512</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 513">Table 513</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 514">Table 514</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 515">Table 515</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 516">Table 516</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 517">Table 517</a> ) </ul><br/> <i>Boosted:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 840">Table 840</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 842">Table 842</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 844">Table 844</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 846">Table 846</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 848">Table 848</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 850">Table 850</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 852">Table 852</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 854">Table 854</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 856">Table 856</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 858">Table 858</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 860">Table 860</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 862">Table 862</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 864">Table 864</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 866">Table 866</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 868">Table 868</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 870">Table 870</a> ) <li>1/SIG*DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 872">Table 872</a> ) <li>DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 874">Table 874</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 876">Table 876</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 878">Table 878</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 880">Table 880</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 882">Table 882</a> ) <li>1/SIG*DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 884">Table 884</a> ) <li>DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 886">Table 886</a> ) <li>SIG (<a href="95758?version=1&table=Table 888">Table 888</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_THAD (<a href="95758?version=1&table=Table 841">Table 841</a> ) <li>DSIG/DPT_THAD (<a href="95758?version=1&table=Table 843">Table 843</a> ) <li>1/SIG*DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 845">Table 845</a> ) <li>DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 847">Table 847</a> ) <li>1/SIG*DSIG/DPT_T1 (<a href="95758?version=1&table=Table 849">Table 849</a> ) <li>DSIG/DPT_T1 (<a href="95758?version=1&table=Table 851">Table 851</a> ) <li>1/SIG*DSIG/DPT_T2 (<a href="95758?version=1&table=Table 853">Table 853</a> ) <li>DSIG/DPT_T2 (<a href="95758?version=1&table=Table 855">Table 855</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 857">Table 857</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 859">Table 859</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 861">Table 861</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 863">Table 863</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 865">Table 865</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 867">Table 867</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 869">Table 869</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 871">Table 871</a> ) <li>1/SIG*DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 873">Table 873</a> ) <li>DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 875">Table 875</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 877">Table 877</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 879">Table 879</a> ) <li>1/SIG*DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 881">Table 881</a> ) <li>DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 883">Table 883</a> ) <li>1/SIG*DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 885">Table 885</a> ) <li>DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 887">Table 887</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DPT_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1029">Table 1029</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1030">Table 1030</a> ) <li>Statistical correlation between DSIG/DABS_Y_THAD and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1031">Table 1031</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1032">Table 1032</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1033">Table 1033</a> ) <li>Statistical correlation between DSIG/DPT_T1 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1034">Table 1034</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1035">Table 1035</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1036">Table 1036</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1037">Table 1037</a> ) <li>Statistical correlation between DSIG/DPT_T2 and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1038">Table 1038</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1039">Table 1039</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1040">Table 1040</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1041">Table 1041</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1042">Table 1042</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1043">Table 1043</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1044">Table 1044</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1045">Table 1045</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1046">Table 1046</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1047">Table 1047</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1048">Table 1048</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1049">Table 1049</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1050">Table 1050</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1051">Table 1051</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1052">Table 1052</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1053">Table 1053</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1054">Table 1054</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1055">Table 1055</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1056">Table 1056</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1057">Table 1057</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1058">Table 1058</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1059">Table 1059</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1060">Table 1060</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1061">Table 1061</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1062">Table 1062</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1063">Table 1063</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1064">Table 1064</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1065">Table 1065</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1066">Table 1066</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1067">Table 1067</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1068">Table 1068</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1069">Table 1069</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1070">Table 1070</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1071">Table 1071</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1072">Table 1072</a> ) <li>Statistical correlation between DSIG/DABS_POUT_TLEP and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1073">Table 1073</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1074">Table 1074</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1075">Table 1075</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1076">Table 1076</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1077">Table 1077</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1078">Table 1078</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1079">Table 1079</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1080">Table 1080</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1081">Table 1081</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1082">Table 1082</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1083">Table 1083</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1084">Table 1084</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1085">Table 1085</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1086">Table 1086</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1087">Table 1087</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1088">Table 1088</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1089">Table 1089</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1090">Table 1090</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1091">Table 1091</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1092">Table 1092</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1093">Table 1093</a> ) <li>Statistical correlation between DSIG/DN_EXTRAJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 1094">Table 1094</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_THAD (<a href="95758?version=1&table=Table 1095">Table 1095</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_Y_THAD (<a href="95758?version=1&table=Table 1096">Table 1096</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_T1 (<a href="95758?version=1&table=Table 1097">Table 1097</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_T2 (<a href="95758?version=1&table=Table 1098">Table 1098</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 1099">Table 1099</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 1100">Table 1100</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1101">Table 1101</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 1102">Table 1102</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DABS_POUT_TLEP (<a href="95758?version=1&table=Table 1103">Table 1103</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 1104">Table 1104</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DN_EXTRAJETS (<a href="95758?version=1&table=Table 1105">Table 1105</a> ) <li>Statistical correlation between DSIG/DN_SUBJETS and DSIG/DN_SUBJETS (<a href="95758?version=1&table=Table 1106">Table 1106</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 889">Table 889</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 890">Table 890</a> ) <li>1/SIG*D2SIG/DPT_THAD/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 891">Table 891</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 898">Table 898</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 899">Table 899</a> ) <li>D2SIG/DPT_THAD/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 900">Table 900</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 1.0 ) (<a href="95758?version=1&table=Table 907">Table 907</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR ( 1.0 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 908">Table 908</a> ) <li>D2SIG/DPT_THAD/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 1.0 ) (<a href="95758?version=1&table=Table 912">Table 912</a> ) <li>D2SIG/DPT_THAD/DABS_Y_TTBAR ( 1.0 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 913">Table 913</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 1.0 ) (<a href="95758?version=1&table=Table 917">Table 917</a> ) <li>1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD ( 1.0 < ABS_Y_THAD < 2.0 ) (<a href="95758?version=1&table=Table 918">Table 918</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 0.0 < ABS_Y_THAD < 1.0 ) (<a href="95758?version=1&table=Table 922">Table 922</a> ) <li>D2SIG/DPT_THAD/DABS_Y_THAD ( 1.0 < ABS_Y_THAD < 2.0 ) (<a href="95758?version=1&table=Table 923">Table 923</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 490.0 GeV < M_TTBAR < 1160.0 GeV) (<a href="95758?version=1&table=Table 927">Table 927</a> ) <li>1/SIG*D2SIG/DPT_THAD/DM_TTBAR ( 1160.0 GeV < M_TTBAR < 3000.0 GeV) (<a href="95758?version=1&table=Table 928">Table 928</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 490.0 GeV < M_TTBAR < 1160.0 GeV) (<a href="95758?version=1&table=Table 932">Table 932</a> ) <li>D2SIG/DPT_THAD/DM_TTBAR ( 1160.0 GeV < M_TTBAR < 3000.0 GeV) (<a href="95758?version=1&table=Table 933">Table 933</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR ( 350.0 GeV < HT_TTBAR < 780.0 GeV) (<a href="95758?version=1&table=Table 937">Table 937</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR ( 780.0 GeV < HT_TTBAR < 2500.0 GeV) (<a href="95758?version=1&table=Table 938">Table 938</a> ) <li>D2SIG/DM_TTBAR/DHT_TTBAR ( 350.0 GeV < HT_TTBAR < 780.0 GeV) (<a href="95758?version=1&table=Table 942">Table 942</a> ) <li>D2SIG/DM_TTBAR/DHT_TTBAR ( 780.0 GeV < HT_TTBAR < 2500.0 GeV) (<a href="95758?version=1&table=Table 943">Table 943</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 947">Table 947</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 948">Table 948</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 949">Table 949</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 40.0 GeV) (<a href="95758?version=1&table=Table 956">Table 956</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 40.0 GeV < PT_TTBAR < 150.0 GeV) (<a href="95758?version=1&table=Table 957">Table 957</a> ) <li>D2SIG/DM_TTBAR/DPT_TTBAR ( 150.0 GeV < PT_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 958">Table 958</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.65 ) (<a href="95758?version=1&table=Table 965">Table 965</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.65 < ABS_Y_TTBAR < 1.3 ) (<a href="95758?version=1&table=Table 966">Table 966</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.3 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 967">Table 967</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.65 ) (<a href="95758?version=1&table=Table 974">Table 974</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 0.65 < ABS_Y_TTBAR < 1.3 ) (<a href="95758?version=1&table=Table 975">Table 975</a> ) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR ( 1.3 < ABS_Y_TTBAR < 2.0 ) (<a href="95758?version=1&table=Table 976">Table 976</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 983">Table 983</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 2.0) (<a href="95758?version=1&table=Table 984">Table 984</a> ) <li>1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 3.0) (<a href="95758?version=1&table=Table 985">Table 985</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 992">Table 992</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS = 2.0) (<a href="95758?version=1&table=Table 993">Table 993</a> ) <li>D2SIG/DPT_THAD/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 3.0) (<a href="95758?version=1&table=Table 994">Table 994</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 1001">Table 1001</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.5) (<a href="95758?version=1&table=Table 1002">Table 1002</a> ) <li>D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.5) (<a href="95758?version=1&table=Table 1006">Table 1006</a> ) <li>D2SIG/DPT_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.5) (<a href="95758?version=1&table=Table 1007">Table 1007</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.0) (<a href="95758?version=1&table=Table 1011">Table 1011</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 1.0) (<a href="95758?version=1&table=Table 1012">Table 1012</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.0) (<a href="95758?version=1&table=Table 1013">Table 1013</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 0.0) (<a href="95758?version=1&table=Table 1020">Table 1020</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS = 1.0) (<a href="95758?version=1&table=Table 1021">Table 1021</a> ) <li>D2SIG/DM_TTBAR/DN_EXTRAJETS (N_EXTRAJETS $\geq$ 2.0) (<a href="95758?version=1&table=Table 1022">Table 1022</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 892">Table 892</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 893">Table 893</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 894">Table 894</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 895">Table 895</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 896">Table 896</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 897">Table 897</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 901">Table 901</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 902">Table 902</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 903">Table 903</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 904">Table 904</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 905">Table 905</a> ) <li>Matrix for D2SIG/DPT_THAD/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 906">Table 906</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 909">Table 909</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 910">Table 910</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 911">Table 911</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 914">Table 914</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 915">Table 915</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 916">Table 916</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 919">Table 919</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 920">Table 920</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 921">Table 921</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 1th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 924">Table 924</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 1th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 925">Table 925</a> ) <li>Matrix for D2SIG/DPT_THAD/DABS_Y_THAD between the 2th and 2th bins of ABS_Y_THAD (<a href="95758?version=1&table=Table 926">Table 926</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 929">Table 929</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 930">Table 930</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 931">Table 931</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 934">Table 934</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 935">Table 935</a> ) <li>Matrix for D2SIG/DPT_THAD/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 936">Table 936</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 1th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 939">Table 939</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 940">Table 940</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 2th bins of HT_TTBAR (<a href="95758?version=1&table=Table 941">Table 941</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 1th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 944">Table 944</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 1th bins of HT_TTBAR (<a href="95758?version=1&table=Table 945">Table 945</a> ) <li>Matrix for D2SIG/DM_TTBAR/DHT_TTBAR between the 2th and 2th bins of HT_TTBAR (<a href="95758?version=1&table=Table 946">Table 946</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 950">Table 950</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 951">Table 951</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 952">Table 952</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 953">Table 953</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 954">Table 954</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 955">Table 955</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 959">Table 959</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 960">Table 960</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 961">Table 961</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 962">Table 962</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 963">Table 963</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 964">Table 964</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 968">Table 968</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 969">Table 969</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 970">Table 970</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 971">Table 971</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 972">Table 972</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 973">Table 973</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 977">Table 977</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 978">Table 978</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 979">Table 979</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 980">Table 980</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 981">Table 981</a> ) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 982">Table 982</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 986">Table 986</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 987">Table 987</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 988">Table 988</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 989">Table 989</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 990">Table 990</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 991">Table 991</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 995">Table 995</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 996">Table 996</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 997">Table 997</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 998">Table 998</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 999">Table 999</a> ) <li>Matrix for D2SIG/DPT_THAD/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1000">Table 1000</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1003">Table 1003</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1004">Table 1004</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1005">Table 1005</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1008">Table 1008</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1009">Table 1009</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1010">Table 1010</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1014">Table 1014</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1015">Table 1015</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1016">Table 1016</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1017">Table 1017</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1018">Table 1018</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1019">Table 1019</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 1th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1023">Table 1023</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1024">Table 1024</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 2th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1025">Table 1025</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 1th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1026">Table 1026</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 2th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1027">Table 1027</a> ) <li>Matrix for D2SIG/DM_TTBAR/DN_EXTRAJETS between the 3th and 3th bins of N_EXTRAJETS (<a href="95758?version=1&table=Table 1028">Table 1028</a> ) </ul><br/> <b>Parton level:</b><br/> <i>Resolved:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 609">Table 609</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 611">Table 611</a> ) <li>1/SIG*DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 613">Table 613</a> ) <li>DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 615">Table 615</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 617">Table 617</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 619">Table 619</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 621">Table 621</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 623">Table 623</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 625">Table 625</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 627">Table 627</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 629">Table 629</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 631">Table 631</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 633">Table 633</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 635">Table 635</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 637">Table 637</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 639">Table 639</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 610">Table 610</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 612">Table 612</a> ) <li>1/SIG*DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 614">Table 614</a> ) <li>DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 616">Table 616</a> ) <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 618">Table 618</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 620">Table 620</a> ) <li>1/SIG*DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 622">Table 622</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 624">Table 624</a> ) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 626">Table 626</a> ) <li>DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 628">Table 628</a> ) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 630">Table 630</a> ) <li>DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 632">Table 632</a> ) <li>1/SIG*DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 634">Table 634</a> ) <li>DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 636">Table 636</a> ) <li>1/SIG*DSIG/DCHI_TT (<a href="95758?version=1&table=Table 638">Table 638</a> ) <li>DSIG/DCHI_TT (<a href="95758?version=1&table=Table 640">Table 640</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DPT_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 799">Table 799</a> ) <li>Statistical correlation between DSIG/DABS_Y_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 800">Table 800</a> ) <li>Statistical correlation between DSIG/DABS_Y_T and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 801">Table 801</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 802">Table 802</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 803">Table 803</a> ) <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 804">Table 804</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 805">Table 805</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 806">Table 806</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 807">Table 807</a> ) <li>Statistical correlation between DSIG/DPT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 808">Table 808</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 809">Table 809</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 810">Table 810</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 811">Table 811</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 812">Table 812</a> ) <li>Statistical correlation between DSIG/DABS_Y_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 813">Table 813</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_T (<a href="95758?version=1&table=Table 814">Table 814</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 815">Table 815</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 816">Table 816</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 817">Table 817</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 818">Table 818</a> ) <li>Statistical correlation between DSIG/DABS_Y_BOOST and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 819">Table 819</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_T (<a href="95758?version=1&table=Table 820">Table 820</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 821">Table 821</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 822">Table 822</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 823">Table 823</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 824">Table 824</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 825">Table 825</a> ) <li>Statistical correlation between DSIG/DHT_TTBAR and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 826">Table 826</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_T (<a href="95758?version=1&table=Table 827">Table 827</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_T (<a href="95758?version=1&table=Table 828">Table 828</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 829">Table 829</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 830">Table 830</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_TTBAR (<a href="95758?version=1&table=Table 831">Table 831</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DABS_Y_BOOST (<a href="95758?version=1&table=Table 832">Table 832</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DHT_TTBAR (<a href="95758?version=1&table=Table 833">Table 833</a> ) <li>Statistical correlation between DSIG/DCHI_TT and DSIG/DCHI_TT (<a href="95758?version=1&table=Table 834">Table 834</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 0.0 < ABS_Y_T < 0.75 ) (<a href="95758?version=1&table=Table 641">Table 641</a> ) <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 0.75 < ABS_Y_T < 1.5 ) (<a href="95758?version=1&table=Table 642">Table 642</a> ) <li>1/SIG*D2SIG/DPT_T/DABS_Y_T ( 1.5 < ABS_Y_T < 2.5 ) (<a href="95758?version=1&table=Table 643">Table 643</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 0.0 < ABS_Y_T < 0.75 ) (<a href="95758?version=1&table=Table 650">Table 650</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 0.75 < ABS_Y_T < 1.5 ) (<a href="95758?version=1&table=Table 651">Table 651</a> ) <li>D2SIG/DPT_T/DABS_Y_T ( 1.5 < ABS_Y_T < 2.5 ) (<a href="95758?version=1&table=Table 652">Table 652</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 659">Table 659</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 180.0 GeV) (<a href="95758?version=1&table=Table 660">Table 660</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 180.0 GeV < PT_TTBAR < 330.0 GeV) (<a href="95758?version=1&table=Table 661">Table 661</a> ) <li>1/SIG*D2SIG/DPT_T/DPT_TTBAR ( 330.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 662">Table 662</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 0.0 GeV < PT_TTBAR < 80.0 GeV) (<a href="95758?version=1&table=Table 673">Table 673</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 80.0 GeV < PT_TTBAR < 180.0 GeV) (<a href="95758?version=1&table=Table 674">Table 674</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 180.0 GeV < PT_TTBAR < 330.0 GeV) (<a href="95758?version=1&table=Table 675">Table 675</a> ) <li>D2SIG/DPT_T/DPT_TTBAR ( 330.0 GeV < PT_TTBAR < 800.0 GeV) (<a href="95758?version=1&table=Table 676">Table 676</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 687">Table 687</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 688">Table 688</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 689">Table 689</a> ) <li>1/SIG*D2SIG/DPT_T/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 690">Table 690</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 701">Table 701</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 702">Table 702</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 703">Table 703</a> ) <li>D2SIG/DPT_T/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 704">Table 704</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 GeV < ABS_Y_TTBAR < 0.5 GeV) (<a href="95758?version=1&table=Table 715">Table 715</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 GeV < ABS_Y_TTBAR < 1.1 GeV) (<a href="95758?version=1&table=Table 716">Table 716</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 GeV < ABS_Y_TTBAR < 1.7 GeV) (<a href="95758?version=1&table=Table 717">Table 717</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 GeV < ABS_Y_TTBAR < 2.5 GeV) (<a href="95758?version=1&table=Table 718">Table 718</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 GeV < ABS_Y_TTBAR < 0.5 GeV) (<a href="95758?version=1&table=Table 729">Table 729</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 GeV < ABS_Y_TTBAR < 1.1 GeV) (<a href="95758?version=1&table=Table 730">Table 730</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 GeV < ABS_Y_TTBAR < 1.7 GeV) (<a href="95758?version=1&table=Table 731">Table 731</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 GeV < ABS_Y_TTBAR < 2.5 GeV) (<a href="95758?version=1&table=Table 732">Table 732</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 743">Table 743</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 744">Table 744</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 745">Table 745</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 746">Table 746</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 325.0 GeV < M_TTBAR < 500.0 GeV) (<a href="95758?version=1&table=Table 757">Table 757</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 500.0 GeV < M_TTBAR < 700.0 GeV) (<a href="95758?version=1&table=Table 758">Table 758</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 700.0 GeV < M_TTBAR < 1000.0 GeV) (<a href="95758?version=1&table=Table 759">Table 759</a> ) <li>D2SIG/DPT_TTBAR/DM_TTBAR ( 1000.0 GeV < M_TTBAR < 2000.0 GeV) (<a href="95758?version=1&table=Table 760">Table 760</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.5 ) (<a href="95758?version=1&table=Table 771">Table 771</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 < ABS_Y_TTBAR < 1.1 ) (<a href="95758?version=1&table=Table 772">Table 772</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 < ABS_Y_TTBAR < 1.7 ) (<a href="95758?version=1&table=Table 773">Table 773</a> ) <li>1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 774">Table 774</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.0 < ABS_Y_TTBAR < 0.5 ) (<a href="95758?version=1&table=Table 785">Table 785</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 0.5 < ABS_Y_TTBAR < 1.1 ) (<a href="95758?version=1&table=Table 786">Table 786</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.1 < ABS_Y_TTBAR < 1.7 ) (<a href="95758?version=1&table=Table 787">Table 787</a> ) <li>D2SIG/DPT_TTBAR/DABS_Y_TTBAR ( 1.7 < ABS_Y_TTBAR < 2.5 ) (<a href="95758?version=1&table=Table 788">Table 788</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 1th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 644">Table 644</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 2th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 645">Table 645</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 2th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 646">Table 646</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 647">Table 647</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 648">Table 648</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DABS_Y_T between the 3th and 3th bins of ABS_Y_T (<a href="95758?version=1&table=Table 649">Table 649</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 1th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 653">Table 653</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 2th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 654">Table 654</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 2th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 655">Table 655</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 1th bins of ABS_Y_T (<a href="95758?version=1&table=Table 656">Table 656</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 2th bins of ABS_Y_T (<a href="95758?version=1&table=Table 657">Table 657</a> ) <li>Matrix for D2SIG/DPT_T/DABS_Y_T between the 3th and 3th bins of ABS_Y_T (<a href="95758?version=1&table=Table 658">Table 658</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 663">Table 663</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 664">Table 664</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 665">Table 665</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 666">Table 666</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 667">Table 667</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 668">Table 668</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 669">Table 669</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 670">Table 670</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 671">Table 671</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 672">Table 672</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 1th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 677">Table 677</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 2th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 678">Table 678</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 2th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 679">Table 679</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 680">Table 680</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 681">Table 681</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 3th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 682">Table 682</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 1th bins of PT_TTBAR (<a href="95758?version=1&table=Table 683">Table 683</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 2th bins of PT_TTBAR (<a href="95758?version=1&table=Table 684">Table 684</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 3th bins of PT_TTBAR (<a href="95758?version=1&table=Table 685">Table 685</a> ) <li>Matrix for D2SIG/DPT_T/DPT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="95758?version=1&table=Table 686">Table 686</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 691">Table 691</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 692">Table 692</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 693">Table 693</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 694">Table 694</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 695">Table 695</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 696">Table 696</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 697">Table 697</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 698">Table 698</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 699">Table 699</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_T/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 700">Table 700</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 705">Table 705</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 706">Table 706</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 707">Table 707</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 708">Table 708</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 709">Table 709</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 710">Table 710</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 711">Table 711</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 712">Table 712</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 713">Table 713</a> ) <li>Matrix for D2SIG/DPT_T/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 714">Table 714</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 719">Table 719</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 720">Table 720</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 721">Table 721</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 722">Table 722</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 723">Table 723</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 724">Table 724</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 725">Table 725</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 726">Table 726</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 727">Table 727</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 728">Table 728</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 733">Table 733</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 734">Table 734</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 735">Table 735</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 736">Table 736</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 737">Table 737</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 738">Table 738</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 739">Table 739</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 740">Table 740</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 741">Table 741</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 742">Table 742</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 747">Table 747</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 748">Table 748</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 749">Table 749</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 750">Table 750</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 751">Table 751</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 752">Table 752</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 753">Table 753</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 754">Table 754</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 755">Table 755</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 756">Table 756</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 1th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 761">Table 761</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 762">Table 762</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 2th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 763">Table 763</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 764">Table 764</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 765">Table 765</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 3th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 766">Table 766</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 1th bins of M_TTBAR (<a href="95758?version=1&table=Table 767">Table 767</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 2th bins of M_TTBAR (<a href="95758?version=1&table=Table 768">Table 768</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 3th bins of M_TTBAR (<a href="95758?version=1&table=Table 769">Table 769</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DM_TTBAR between the 4th and 4th bins of M_TTBAR (<a href="95758?version=1&table=Table 770">Table 770</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 775">Table 775</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 776">Table 776</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 777">Table 777</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 778">Table 778</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 779">Table 779</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 780">Table 780</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 781">Table 781</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 782">Table 782</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 783">Table 783</a> ) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 784">Table 784</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 1th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 789">Table 789</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 790">Table 790</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 2th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 791">Table 791</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 792">Table 792</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 793">Table 793</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 3th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 794">Table 794</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 1th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 795">Table 795</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 2th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 796">Table 796</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 3th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 797">Table 797</a> ) <li>Matrix for D2SIG/DPT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="95758?version=1&table=Table 798">Table 798</a> ) </ul><br/> <i>Resolved with CMS binning:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 835">Table 835</a> ) <li>DSIG/DY_T (<a href="95758?version=1&table=Table 836">Table 836</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 837">Table 837</a> ) <li>DSIG/DPT_TTBAR (<a href="95758?version=1&table=Table 838">Table 838</a> ) <li>DSIG/DY_TTBAR (<a href="95758?version=1&table=Table 839">Table 839</a> ) </ul><br/> <i>Boosted:</i><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1107">Table 1107</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1109">Table 1109</a> ) <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 1111">Table 1111</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 1113">Table 1113</a> ) <li>SIG (<a href="95758?version=1&table=Table 1115">Table 1115</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>1/SIG*DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1108">Table 1108</a> ) <li>DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1110">Table 1110</a> ) <li>1/SIG*DSIG/DPT_T (<a href="95758?version=1&table=Table 1112">Table 1112</a> ) <li>DSIG/DPT_T (<a href="95758?version=1&table=Table 1114">Table 1114</a> ) </ul><br/> Inter-spectra correlations:<br/> <ul><br/> <li>Statistical correlation between DSIG/DM_TTBAR and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1126">Table 1126</a> ) <li>Statistical correlation between DSIG/DPT_T and DSIG/DM_TTBAR (<a href="95758?version=1&table=Table 1127">Table 1127</a> ) <li>Statistical correlation between DSIG/DPT_T and DSIG/DPT_T (<a href="95758?version=1&table=Table 1128">Table 1128</a> ) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li>1/SIG*D2SIG/DM_TTBAR/DPT_T ( 350.0 GeV < PT_T < 550.0 GeV) (<a href="95758?version=1&table=Table 1116">Table 1116</a> ) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T ( 550.0 GeV < PT_T < 2000.0 GeV) (<a href="95758?version=1&table=Table 1117">Table 1117</a> ) <li>D2SIG/DM_TTBAR/DPT_T ( 350.0 GeV < PT_T < 550.0 GeV) (<a href="95758?version=1&table=Table 1121">Table 1121</a> ) <li>D2SIG/DM_TTBAR/DPT_T ( 550.0 GeV < PT_T < 2000.0 GeV) (<a href="95758?version=1&table=Table 1122">Table 1122</a> ) </ul><br/> Covariances:<br/> <ul><br/> <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 1th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1118">Table 1118</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 2th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1119">Table 1119</a> ) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T between the 2th and 2th bins of PT_T (<a href="95758?version=1&table=Table 1120">Table 1120</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 1th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1123">Table 1123</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 2th and 1th bins of PT_T (<a href="95758?version=1&table=Table 1124">Table 1124</a> ) <li>Matrix for D2SIG/DM_TTBAR/DPT_T between the 2th and 2th bins of PT_T (<a href="95758?version=1&table=Table 1125">Table 1125</a> ) </ul><br/>
Covariance matrix of the Relative differential cross-section as function of $p_{T}^{t\bar{t}}$ at particle level in the resolved topology, accounting for the statistical and systematic uncertainties.
The production of a prompt photon in association with a $Z$ boson is studied in proton-proton collisions at a centre-of-mass energy $\sqrt{s} =$ 13 TeV. The analysis uses a data sample with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at the LHC from 2015 to 2018. The production cross-section for the process $pp \rightarrow \ell^+\ell^-\gamma+X$ ($\ell = e, \mu$) is measured within a fiducial phase-space region defined by kinematic requirements on the photon and the leptons, and by isolation requirements on the photon. An experimental precision of 2.9% is achieved for the fiducial cross-section. Differential cross-sections are measured as a function of each of six kinematic variables characterising the $\ell^+\ell^-\gamma$ system. The data are compared with theoretical predictions based on next-to-leading-order and next-to-next-to-leading-order perturbative QCD calculations. The impact of next-to-leading-order electroweak corrections is also considered.
The measured fiducial cross section. "Uncor" uncertainty includes all systematic uncertainties that are uncorrelated between electron and muon channels such as the uncertainty on the electron identification efficiency and the uncorrelated component of the background uncertainties. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production of 4.57 fb.
The measured fiducial cross section. "Uncor" uncertainty includes all systematic uncertainties that are uncorrelated between electron and muon channels such as the uncertainty on the electron identification efficiency and the uncorrelated component of the background uncertainties. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with Sherpa 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production of 4.57 fb.
The measured fiducial cross section vs $E_{\mathrm{T}}^\gamma$. The central values are provided along with the statistical and systematic uncertainties together with the sign information. The statistical and "Uncor" uncertainty should be treated as uncorrelated bin-to-bin, while the rest are correlated between bins, and they are written as signed NP variations. The parton-to-particle correction factor $C_{theory}$ is the ratio of the cross-section predicted by Sherpa LO samples at particle level within the fiducial phase-space region defined in Table 4 to the predicted cross-section at parton level within the same fiducial region but with the smooth-cone isolation prescription defined above replacing the particle-level photon isolation criterion, and with Born-level leptons in place of dressed leptons. This correction should be applied on fixed order parton-level calculations. The systematic uncertainty is evaluated from a comparison with the correction factor obtained using events generated with SHERPA 2.2.2 at NLO. In the case that the calculations are valid for dressed leptons, a modified correction factor excluding the Born-to-dressed lepton correction should be applied instead. This correction only takes into account the particle-level isolation criteria, and is provided separately here. The Sherpa 2.2.8 NLO cross-sections given below include a small contribution from EW $Z\gamma jj$ production.
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