A measurement of the top-quark mass ($m_t$) in the $t\bar{t}\rightarrow~\textrm{lepton}+\textrm{jets}$ channel is presented, with an experimental technique which exploits semileptonic decays of $b$-hadrons produced in the top-quark decay chain. The distribution of the invariant mass $m_{\ell\mu}$ of the lepton, $\ell$ (with $\ell=e,\mu$), from the $W$-boson decay and the muon, $\mu$, originating from the $b$-hadron decay is reconstructed, and a binned-template profile likelihood fit is performed to extract $m_t$. The measurement is based on data corresponding to an integrated luminosity of 36.1 fb$^{-1}$ of $\sqrt{s} = 13~\textrm{TeV}$$pp$ collisions provided by the Large Hadron Collider and recorded by the ATLAS detector. The measured value of the top-quark mass is $m_{t} = 174.41\pm0.39~(\textrm{stat.})\pm0.66~(\textrm{syst.})\pm0.25~(\textrm{recoil})~\textrm{GeV}$, where the third uncertainty arises from changing the PYTHIA8 parton shower gluon-recoil scheme, used in top-quark decays, to a recently developed setup.
Top mass measurement result.
List of all the individual sources of systematic uncertainty considered in the analysis. The individual sources, each corresponding to an independent nuisance parameter in the fit, are grouped into categories, as indicated in the first column. The second column shows the impact of each of the individual sources on the measurement, obtained as the shift on the top mass induced by a positive shift of the each of the nuisance parameters by its post-fit uncertainty. Sources for which no impact is indicated are neglected in the fit procedure as their impact on the total prediction is negligible in any of the bins. The last column shows the statistical uncertainty in each of the reported numbers as estimated with the bootstrap method.
Ranking, from top to bottom, of the main systematic uncertainties (excluding recoil) showing the pulls and the impact of the systematic uncertainties on the top mass, from the combined opposite sign (OS) and same sign (SS) binned-template profile likelihood fit to data. The OS or SS refers to the charge signs of the primary lepton and the soft muon. The gamma parameters are NPs used to describe the effect of the limited statistics of the sample.
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb$^{-1}$ of $\sqrt{s}=13$ TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015-2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single $Z$ boson production, Higgs boson production and on-shell $ZZ$ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The $Z\rightarrow 4\ell$ branching fraction is extracted, giving a value of $\left(4.41 \pm 0.30\right) \times 10^{-6}$. Constraints on effective field theory parameters and a model based on a spontaneously broken $B-L$ gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information.
Inclusive differential cross section for four leptons (Max = 1710~GeV).
Inclusive differential cross section for four muons (Max = 1320~GeV)
Inclusive differential cross section for four electrons (Max = 887~GeV).
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.
Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-muon category.
Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 2e2mu category.
Distribution of the four-lepton invariant mass in the four-lepton final state for the ggF-MVA-high 4-electron category.
A search is presented for the production of the Standard Model Higgs boson in association with a high-energy photon. With a focus on the vector-boson fusion process and the dominant Higgs boson decay into $b$-quark pairs, the search benefits from a large reduction of multijet background compared to more inclusive searches. Results are reported from the analysis of 132 fb$^{-1}$ of $pp$ collision data at $\sqrt{s}$=13 TeV collected with the ATLAS detector at the LHC. The measured Higgs boson signal yield in this final-state signature is $1.3 \pm 1.0$ times the Standard Model prediction. The observed significance of the Higgs boson signal above the background is 1.3 standard deviations, compared to an expected significance of 1.0 standard deviations.
Comparisons of data and simulated event distributions of the BDT input variable \(\Delta \eta_{jj}\) in the two \(m_{bb}\) sidebands after kinematic reweighting of the non-resonant \(b\bar{b}\gamma jj\) background. The data are shown as black points, and the background contributions are stacked in coloured histograms. The Higgs boson signal contribution is scaled up and represented by the dashed red line. The bottom panel in each plot shows the ratio of the data to the SM prediction, where the uncertainty band corresponds to the statistical uncertainty only.
Comparisons of data and simulated event distributions of the BDT input variable \(p_{\text{T}}^{\text{balance}}\) in the two \(m_{bb}\) sidebands after kinematic reweighting of the non-resonant \(b\bar{b}\gamma jj\) background. The data are shown as black points, and the background contributions are stacked in coloured histograms. The Higgs boson signal contribution is scaled up and represented by the dashed red line. The bottom panel in each plot shows the ratio of the data to the SM prediction, where the uncertainty band corresponds to the statistical uncertainty only.
The \(m_{bb}\) distributions in the HighBDT categories, overlaid with contributions from the \(H\gamma jj\) signal as well as the resonant \(Z\gamma jj\) and non-resonant \(b\bar{b} \gamma jj\) background fits. The combined \(\chi^2\) per degree of freedom is \(45.2/45\). The bottom panel in each plot presents the significance of the Higgs boson signal relative to the non-resonant \(b\bar{b} \gamma jj\) background in each bin.
A search for pair production of bottom squarks in events with hadronically decaying $\tau$-leptons, $b$-tagged jets and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at $\sqrt{s}$ = 13 TeV delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of 139 fb$^{-1}$. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino $\tilde \chi_2^0$ and a bottom quark, with $\tilde \chi_2^0$ decaying into a Higgs boson and the lightest neutralino $\tilde \chi_1^0$. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying $\tau$-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the $\tilde \chi_2^0$, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between $\tilde \chi_2^0$ and $\tilde \chi_1^0$. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model.
The expected exclusion contour at $95\%$ CL as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Masses within the contour are excluded.
The observed exclusion contour at $95\%$ CL as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Masses within the contour are excluded.
Acceptance in the Single-bin SR as a function of the M(Sbottom) vs. M(N2) with the $\Delta M$(N2,N1) = 130 GeV. Keep in mind that the acceptance is given in units of $10^{-4}$.
A search for supersymmetry in events with four or more charged leptons (electrons, muons and $\tau$-leptons) is presented. The analysis uses a data sample corresponding to $139\,\mbox{fb\(^{-1}\)}$ of proton-proton collisions delivered by the Large Hadron Collider at $\sqrt{s}=13$ TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying $\tau$-leptons are designed to target several supersymmetric models, while a general five-lepton signal region targets any new physics phenomena leading to a final state with five charged leptons. Data yields are consistent with Standard Model expectations and results are used to set upper limits on contributions from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of general gauge-mediated supersymmetry, excluding higgsino masses up to $540$ GeV. In $R$-parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of $1.6$ TeV, $1.2$ TeV, and $2.5$ TeV are placed on wino, slepton and gluino masses, respectively.
The $E_{\mathrm{T}}^{\mathrm{miss}}$ distribution in SR0-ZZ$^{\mathrm{loose}}$ and SR0-ZZ$^{\mathrm{tight}}$ for events passing the signal region requirements except the $E_{\mathrm{T}}^{\mathrm{miss}}$ requirement. Distributions for data, the estimated SM backgrounds after the background-only fit, and an example SUSY scenario are shown. "Other" is the sum of the $tWZ$, $t\bar{t}WW$, $t\bar{t} ZZ$, $t\bar{t} WH$, $t\bar{t} HH$, $t\bar{t} tW$, and $t\bar{t}t\bar{t}$ backgrounds. The last bin captures the overflow events. The lower panel shows the ratio of the observed data to the expected SM background yield in each bin. Both the statistical and systematic uncertainties in the SM background are included in the shaded band. The red arrows indicate the $E_{\mathrm{T}}^{\mathrm{miss}}$ selections in the signal regions.
The $E_{\mathrm{T}}^{\mathrm{miss}}$ distribution in SR0-ZZ$_{\mathrm{bveto}}^{\mathrm{loose}}$ and SR0-ZZ$_{\mathrm{bveto}}^{\mathrm{tight}}$ for events passing the signal region requirements except the $E_{\mathrm{T}}^{\mathrm{miss}}$ requirement. Distributions for data, the estimated SM backgrounds after the background-only fit, and an example SUSY scenario are shown. "Other" is the sum of the $tWZ$, $t\bar{t}WW$, $t\bar{t} ZZ$, $t\bar{t} WH$, $t\bar{t} HH$, $t\bar{t} tW$, and $t\bar{t}t\bar{t}$ backgrounds. The last bin captures the overflow events. The lower panel shows the ratio of the observed data to the expected SM background yield in each bin. Both the statistical and systematic uncertainties in the SM background are included in the shaded band. The red arrows indicate the $E_{\mathrm{T}}^{\mathrm{miss}}$ selections in the signal regions.
The $E_{\mathrm{T}}^{\mathrm{miss}}$ distribution in SR5L. Distributions for data, the estimated SM backgrounds after the background-only fit, and an example SUSY scenario are shown. "Other" is the sum of the $tWZ$, $t\bar{t}WW$, $t\bar{t} ZZ$, $t\bar{t} WH$, $t\bar{t} HH$, $t\bar{t} tW$, and $t\bar{t}t\bar{t}$ backgrounds. The last bin captures the overflow events. The lower panel shows the ratio of the observed data to the expected SM background yield in each bin. Both the statistical and systematic uncertainties in the SM background are included in the shaded band.
Exclusive dimuon production in ultraperipheral collisions (UPC), resulting from photon-photon interactions in the strong electromagnetic fields of colliding high-energy lead nuclei, $\mathrm{PbPb}(\gamma\gamma) \rightarrow \mu^+\mu^- (\mathrm{Pb}^{(\star)}\mathrm{Pb}^{(\star)} )$, is studied using $\mathcal{L}_{\mathrm{int}} = 0.48$ nb$^{-1}$ of $\sqrt{s_\mathrm{NN}}=5.02$ TeV lead-lead collision data at the LHC with the ATLAS detector. Dimuon pairs are measured in the fiducial region $p_{\mathrm{T}\mu} > 4$ GeV, $|\eta_{\mu}| < 2.4$, invariant mass $m_{\mu\mu} > 10$ GeV, and $p_{\mathrm{T,\mu\mu}} < 2$ GeV. The primary background from single-dissociative processes is extracted from the data using a template fitting technique. Differential cross sections are presented as a function of $m_{\mu\mu}$, absolute pair rapidity ($|y_{\mu\mu}|$), scattering angle in the dimuon rest frame ($|\cos \vartheta^{\star}_{\mu\mu}|$) and the colliding photon energies. The total cross section of the UPC $\gamma \gamma \rightarrow \mu^{+}\mu^{-}$ process in the fiducial volume is measured to be $\sigma_{\mathrm{fid}}^{\mu\mu} = 34.1 \! \pm \! 0.3 \mathrm{(stat.)} \! \pm \! 0.7 \mathrm{(syst.)}$ $\mu\mathrm{b}$. Generally good agreement is found with calculations from STARlight, which incorporate the leading-order Breit-Wheeler process with no final-state effects, albeit differences between the measurements and theoretical expectations are observed. In particular, the measured cross sections at larger $|y_{\mu\mu}|$ are found to be about 10-20% larger in data than in the calculations, suggesting the presence of larger fluxes of photons in the initial state. Modification of the dimuon cross sections in the presence of forward and/or backward neutron production is also studied and is found to be associated with a harder incoming photon spectrum, consistent with expectations.
Differential UPC dimuon cross sections shown as a function of $|y_{\mu\mu}|$ in the interval $10 < |m_{\mu\mu}| < 20$ GeV.
Differential UPC dimuon cross sections shown as a function of $|y_{\mu\mu}|$ in the interval $20 < |m_{\mu\mu}| < 40$ GeV.
Differential UPC dimuon cross sections shown as a function of $|y_{\mu\mu}|$ in the interval $40 < |m_{\mu\mu}| < 80$ GeV.
Measurements of both the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a $Z$ boson ($t\bar{t}Z$) are presented. The measurements are performed by targeting final states with three or four isolated leptons (electrons or muons) and are based on $\sqrt{s} = 13$ TeV proton-proton collision data with an integrated luminosity of 139 fb$^{-1}$, recorded from 2015 to 2018 with the ATLAS detector at the CERN Large Hadron Collider. The inclusive cross section is measured to be $\sigma_{t\bar{t}Z} = 0.99 \pm 0.05$ (stat.) $\pm 0.08$ (syst.) pb, in agreement with the most precise theoretical predictions. The differential measurements are presented as a function of a number of kinematic variables which probe the kinematics of the $t\bar{t}Z$ system. Both absolute and normalised differential cross-section measurements are performed at particle and parton levels for specific fiducial volumes and are compared with theoretical predictions at different levels of precision, based on a $\chi^{2}/$ndf and $p$-value computation. Overall, good agreement is observed between the unfolded data and the predictions.
The measured $t\bar{t}\text{Z}$ cross-section value and its uncertainty based on the fit results from the combined trilepton and tetralepton channels. The value corresponds to the phase-space region where the difermion mass from the Z boson decay lies in the range $70 < m_{f\bar{f}} < 110$ GeV.
List of relative uncertainties of the measured inclusive $t\bar{t}\text{Z}$ cross section from the combined fit. The uncertainties are symmetrised for presentation and grouped into the categories described in the text. The quadratic sum of the individual uncertainties is not equal to the total uncertainty due to correlations introduced by the fit.
The definitions of the trilepton signal regions: for the inclusive measurement, a combination of the regions with pseudo-continuous $b$-tagging 3$\ell$-Z-1$b$4$j$-PCBT and 3$\ell$-Z-2$b$3$j$-PCBT is used, whereas for the differential measurement, only the region 3$\ell$-Z-2$b$3$j$, with a fixed $b$-tagging WP is employed.
A search is performed for the electroweak pair production of charginos and associated production of a chargino and neutralino, each of which decays through an $R$-parity-violating coupling into a lepton and a $W$, $Z$, or Higgs boson. The trilepton invariant-mass spectrum is constructed from events with three or more leptons, targeting chargino decays that include an electron or muon and a leptonically decaying $Z$ boson. The analyzed dataset corresponds to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collision data produced by the Large Hadron Collider at a center-of-mass energy of $\sqrt{s}$ = 13 TeV and collected by the ATLAS experiment between 2015 and 2018. The data are found to be consistent with predictions from the Standard Model. The results are interpreted as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model. Limits are also set on the production of charginos and neutralinos for a Minimal Supersymmetric Standard Model with an approximate $B$-$L$ symmetry. Charginos and neutralinos with masses between 100 GeV and 1100 GeV are excluded depending on the assumed decay branching fractions into a lepton (electron, muon, or $\tau$-lepton) plus a boson ($W$, $Z$, or Higgs).
This is the HEPData space for the trilepton resonance wino search, the full resolution figures can be found here https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/SUSY-2018-36/. The full statistical likelihoods have been provided for this analysis. They can be downloaded by clicking on the purple 'Resources' buttun above where they can then be found in the 'Common Resources' area. A detailed README for how to use the likelihoods is also included in this download. <b>Exclusion contours:</b> <ul display="inline-block"> <li><a href="?table=Obs.%20data%20vs%20SM%20bkg.%20exp.%20in%20CRs%20and%20VRs">Obs. data vs SM bkg. exp. in CRs and VRs</a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Obs_0%20">$\ell=(e, \mu, \tau)$, Obs_0 </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up%20">$\ell=(e, \mu, \tau)$, Obs_0_Up </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down%20">$\ell=(e, \mu, \tau)$, Obs_0_Down </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Exp_0%20">$\ell=(e, \mu, \tau)$, Exp_0 </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up%20">$\ell=(e, \mu, \tau)$, Exp_0_Up </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down%20">$\ell=(e, \mu, \tau)$, Exp_0_Down </a> <li><a href="?table=$\ell=e$,%20Obs_0%20">$\ell=e$, Obs_0 </a> <li><a href="?table=$\ell=e$,%20Obs_0_Up%20">$\ell=e$, Obs_0_Up </a> <li><a href="?table=$\ell=e$,%20Obs_0_Down%20">$\ell=e$, Obs_0_Down </a> <li><a href="?table=$\ell=e$,%20Exp_0%20">$\ell=e$, Exp_0 </a> <li><a href="?table=$\ell=e$,%20Exp_0_Up%20">$\ell=e$, Exp_0_Up </a> <li><a href="?table=$\ell=e$,%20Exp_0_Down%20">$\ell=e$, Exp_0_Down </a> <li><a href="?table=$\ell=\mu$,%20Obs_0%20">$\ell=\mu$, Obs_0 </a> <li><a href="?table=$\ell=\mu$,%20Obs_0_Up%20">$\ell=\mu$, Obs_0_Up </a> <li><a href="?table=$\ell=\mu$,%20Obs_0_Down%20">$\ell=\mu$, Obs_0_Down </a> <li><a href="?table=$\ell=\mu$,%20Exp_0%20">$\ell=\mu$, Exp_0 </a> <li><a href="?table=$\ell=\mu$,%20Exp_0_Up%20">$\ell=\mu$, Exp_0_Up </a> <li><a href="?table=$\ell=\mu$,%20Exp_0_Down%20">$\ell=\mu$, Exp_0_Down </a> <li><a href="?table=$\ell=\tau$,%20Obs_0%20">$\ell=\tau$, Obs_0 </a> <li><a href="?table=$\ell=\tau$,%20Obs_0_Up%20">$\ell=\tau$, Obs_0_Up </a> <li><a href="?table=$\ell=\tau$,%20Obs_0_Down%20">$\ell=\tau$, Obs_0_Down </a> <li><a href="?table=$\ell=\tau$,%20Exp_0%20">$\ell=\tau$, Exp_0 </a> <li><a href="?table=$\ell=\tau$,%20Exp_0_Up%20">$\ell=\tau$, Exp_0_Up </a> <li><a href="?table=$\ell=\tau$,%20Exp_0_Down%20">$\ell=\tau$, Exp_0_Down </a> </ul> <b>Triangle Exclusion contours:</b> <ul display="inline-block"> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs%20Lim">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Obs Lim</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp%20Lim">Triangle, 600 GeV, $\ell=(e, \mu, \tau)$, Exp Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs%20Lim">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Obs Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp%20Lim">Triangle, 700 GeV, $\ell=(e, \mu, \tau)$, Exp Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs%20Lim">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Obs Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp%20Lim">Triangle, 800 GeV, $\ell=(e, \mu, \tau)$, Exp Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs%20Lim">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Obs Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp%20Lim">Triangle, 900 GeV, $\ell=(e, \mu, \tau)$, Exp Lim</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Obs_0">Triangle, 600 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, 600 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, 600 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Exp_0">Triangle, 600 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, 600 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, 600 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Obs%20Lim">Triangle, 600 GeV, $\ell=e$, Obs Lim</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=e$,%20Exp%20Lim">Triangle, 600 GeV, $\ell=e$, Exp Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Obs_0">Triangle, 700 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, 700 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, 700 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Exp_0">Triangle, 700 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, 700 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, 700 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Obs%20Lim">Triangle, 700 GeV, $\ell=e$, Obs Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=e$,%20Exp%20Lim">Triangle, 700 GeV, $\ell=e$, Exp Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Obs_0">Triangle, 800 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, 800 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, 800 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Exp_0">Triangle, 800 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, 800 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, 800 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Obs%20Lim">Triangle, 800 GeV, $\ell=e$, Obs Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=e$,%20Exp%20Lim">Triangle, 800 GeV, $\ell=e$, Exp Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Obs_0">Triangle, 900 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, 900 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, 900 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Exp_0">Triangle, 900 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, 900 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, 900 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Obs%20Lim">Triangle, 900 GeV, $\ell=e$, Obs Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=e$,%20Exp%20Lim">Triangle, 900 GeV, $\ell=e$, Exp Lim</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, 600 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, 600 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, 600 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, 600 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, 600 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, 600 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Obs%20Lim">Triangle, 600 GeV, $\ell=\mu$, Obs Lim</a> <li><a href="?table=Triangle,%20600%20GeV,%20$\ell=\mu$,%20Exp%20Lim">Triangle, 600 GeV, $\ell=\mu$, Exp Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, 700 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, 700 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, 700 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, 700 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, 700 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, 700 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Obs%20Lim">Triangle, 700 GeV, $\ell=\mu$, Obs Lim</a> <li><a href="?table=Triangle,%20700%20GeV,%20$\ell=\mu$,%20Exp%20Lim">Triangle, 700 GeV, $\ell=\mu$, Exp Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, 800 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, 800 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, 800 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, 800 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, 800 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, 800 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Obs%20Lim">Triangle, 800 GeV, $\ell=\mu$, Obs Lim</a> <li><a href="?table=Triangle,%20800%20GeV,%20$\ell=\mu$,%20Exp%20Lim">Triangle, 800 GeV, $\ell=\mu$, Exp Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, 900 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, 900 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, 900 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, 900 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, 900 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, 900 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Obs%20Lim">Triangle, 900 GeV, $\ell=\mu$, Obs Lim</a> <li><a href="?table=Triangle,%20900%20GeV,%20$\ell=\mu$,%20Exp%20Lim">Triangle, 900 GeV, $\ell=\mu$, Exp Lim</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Obs_0">Triangle, 200 GeV, $\ell=\tau$, Obs_0</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Obs_0_Up">Triangle, 200 GeV, $\ell=\tau$, Obs_0_Up</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Obs_0_Down">Triangle, 200 GeV, $\ell=\tau$, Obs_0_Down</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Exp_0">Triangle, 200 GeV, $\ell=\tau$, Exp_0</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Exp_0_Up">Triangle, 200 GeV, $\ell=\tau$, Exp_0_Up</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Exp_0_Down">Triangle, 200 GeV, $\ell=\tau$, Exp_0_Down</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Obs%20Lim">Triangle, 200 GeV, $\ell=\tau$, Obs Lim</a> <li><a href="?table=Triangle,%20200%20GeV,%20$\ell=\tau$,%20Exp%20Lim">Triangle, 200 GeV, $\ell=\tau$, Exp Lim</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Obs_0">Triangle, 300 GeV, $\ell=\tau$, Obs_0</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Obs_0_Up">Triangle, 300 GeV, $\ell=\tau$, Obs_0_Up</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Obs_0_Down">Triangle, 300 GeV, $\ell=\tau$, Obs_0_Down</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Exp_0">Triangle, 300 GeV, $\ell=\tau$, Exp_0</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Exp_0_Up">Triangle, 300 GeV, $\ell=\tau$, Exp_0_Up</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Exp_0_Down">Triangle, 300 GeV, $\ell=\tau$, Exp_0_Down</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Obs%20Lim">Triangle, 300 GeV, $\ell=\tau$, Obs Lim</a> <li><a href="?table=Triangle,%20300%20GeV,%20$\ell=\tau$,%20Exp%20Lim">Triangle, 300 GeV, $\ell=\tau$, Exp Lim</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Obs_0">Triangle, 400 GeV, $\ell=\tau$, Obs_0</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Obs_0_Up">Triangle, 400 GeV, $\ell=\tau$, Obs_0_Up</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Obs_0_Down">Triangle, 400 GeV, $\ell=\tau$, Obs_0_Down</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Exp_0">Triangle, 400 GeV, $\ell=\tau$, Exp_0</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Exp_0_Up">Triangle, 400 GeV, $\ell=\tau$, Exp_0_Up</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Exp_0_Down">Triangle, 400 GeV, $\ell=\tau$, Exp_0_Down</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Obs%20Lim">Triangle, 400 GeV, $\ell=\tau$, Obs Lim</a> <li><a href="?table=Triangle,%20400%20GeV,%20$\ell=\tau$,%20Exp%20Lim">Triangle, 400 GeV, $\ell=\tau$, Exp Lim</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Obs_0">Triangle, 500 GeV, $\ell=\tau$, Obs_0</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Obs_0_Up">Triangle, 500 GeV, $\ell=\tau$, Obs_0_Up</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Obs_0_Down">Triangle, 500 GeV, $\ell=\tau$, Obs_0_Down</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Exp_0">Triangle, 500 GeV, $\ell=\tau$, Exp_0</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Exp_0_Up">Triangle, 500 GeV, $\ell=\tau$, Exp_0_Up</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Exp_0_Down">Triangle, 500 GeV, $\ell=\tau$, Exp_0_Down</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Obs%20Lim">Triangle, 500 GeV, $\ell=\tau$, Obs Lim</a> <li><a href="?table=Triangle,%20500%20GeV,%20$\ell=\tau$,%20Exp%20Lim">Triangle, 500 GeV, $\ell=\tau$, Exp Lim</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ObsLimVal">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, ObsLimVal</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ExpLimVal">Triangle, SRFR, 700 GeV, $\ell=(e, \mu, \tau)$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ObsLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ExpLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Obs_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20Exp_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ObsLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=(e,%20\mu,%20\tau)$,%20ExpLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=(e, \mu, \tau)$, ExpLimVal</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Obs_0">Triangle, SRFR, 700 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, SRFR, 700 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, SRFR, 700 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Exp_0">Triangle, SRFR, 700 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, SRFR, 700 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, SRFR, 700 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20ObsLimVal">Triangle, SRFR, 700 GeV, $\ell=e$, ObsLimVal</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=e$,%20ExpLimVal">Triangle, SRFR, 700 GeV, $\ell=e$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20ObsLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=e$,%20ExpLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=e$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Obs_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Obs_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Exp_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20Exp_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20ObsLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=e$,%20ExpLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=e$, ExpLimVal</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, SRFR, 700 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, SRFR, 700 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, SRFR, 700 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, SRFR, 700 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, SRFR, 700 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, SRFR, 700 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20ObsLimVal">Triangle, SRFR, 700 GeV, $\ell=\mu$, ObsLimVal</a> <li><a href="?table=Triangle,%20SRFR,%20700%20GeV,%20$\ell=\mu$,%20ExpLimVal">Triangle, SRFR, 700 GeV, $\ell=\mu$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20ObsLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR4$\ell$,%20700%20GeV,%20$\ell=\mu$,%20ExpLimVal">Triangle, SR4$\ell$, 700 GeV, $\ell=\mu$, ExpLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Obs_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Obs_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Obs_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Obs_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Exp_0</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Up">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Exp_0_Up</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20Exp_0_Down">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, Exp_0_Down</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20ObsLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, ObsLimVal</a> <li><a href="?table=Triangle,%20SR3$\ell$,%20700%20GeV,%20$\ell=\mu$,%20ExpLimVal">Triangle, SR3$\ell$, 700 GeV, $\ell=\mu$, ExpLimVal</a> </ul> <b>Upper limits:</b> <ul display="inline-block"> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20upperLimit_XS_gr%20">$\ell=(e, \mu, \tau)$, upperLimit_XS_gr </a> <li><a href="?table=$\ell=(e,%20\mu,%20\tau)$,%20expectedUpperLimit_XS_gr%20">$\ell=(e, \mu, \tau)$, expectedUpperLimit_XS_gr </a> <li><a href="?table=$\ell=e$,%20upperLimit_XS_gr%20">$\ell=e$, upperLimit_XS_gr </a> <li><a href="?table=$\ell=e$,%20expectedUpperLimit_XS_gr%20">$\ell=e$, expectedUpperLimit_XS_gr </a> <li><a href="?table=$\ell=\mu$,%20upperLimit_XS_gr%20">$\ell=\mu$, upperLimit_XS_gr </a> <li><a href="?table=$\ell=\mu$,%20expectedUpperLimit_XS_gr%20">$\ell=\mu$, expectedUpperLimit_XS_gr </a> <li><a href="?table=$\ell=\tau$,%20upperLimit_XS_gr%20">$\ell=\tau$, upperLimit_XS_gr </a> <li><a href="?table=$\ell=\tau$,%20expectedUpperLimit_XS_gr%20">$\ell=\tau$, expectedUpperLimit_XS_gr </a> </ul> <b>Kinematic distributions:</b> <ul display="inline-block"> <li><a href="?table=Variable%20bin%20$m_{Z\ell}$%20for%20SRFR%20">Variable bin $m_{Z\ell}$ for SRFR </a> <li><a href="?table=Variable%20bin%20$m_{Z\ell}$%20for%20SR4$\ell$%20">Variable bin $m_{Z\ell}$ for SR4$\ell$ </a> <li><a href="?table=Variable%20bin%20$m_{Z\ell}$%20for%20SR3$\ell$%20">Variable bin $m_{Z\ell}$ for SR3$\ell$ </a> <li><a href="?table=N-1%20for%20SR3$\ell$,%20$E^{miss}_{T}$%20">N-1 for SR3$\ell$, $E^{miss}_{T}$ </a> <li><a href="?table=N-1%20for%20SR3$\ell$,%20$m^{min}_{T}$%20">N-1 for SR3$\ell$, $m^{min}_{T}$ </a> <li><a href="?table=N-1%20for%20SR4$\ell$,%20$E^{miss,SF}_{T}$%20">N-1 for SR4$\ell$, $E^{miss,SF}_{T}$ </a> <li><a href="?table=N-1%20for%20SRFR,%20$m^{asym}_{Z\ell}$%20">N-1 for SRFR, $m^{asym}_{Z\ell}$ </a> <li><a href="?table=$m_{Z\ell}$%20for%20SRFR%20">$m_{Z\ell}$ for SRFR </a> <li><a href="?table=$m_{Z\ell}$%20for%20SR4$\ell$%20">$m_{Z\ell}$ for SR4$\ell$ </a> <li><a href="?table=$m_{Z\ell}$%20for%20SR3$\ell$%20">$m_{Z\ell}$ for SR3$\ell$ </a> <li><a href="?table=$L_{T}$%20for%20SR4$\ell$%20">$L_{T}$ for SR4$\ell$ </a> </ul> <b>Cut flows:</b> <ul display="inline-block"> <li><a href="?table=Yields%20Table">Yields Table</a> <li><a href="?table=Model-Independent%20Results%20Table,%20SRFR">Model-Independent Results Table, SRFR</a> <li><a href="?table=Model-Independent%20Results%20Table,%20SR4$\ell$">Model-Independent Results Table, SR4$\ell$</a> <li><a href="?table=Model-Independent%20Results%20Table,%20SR3$\ell$">Model-Independent Results Table, SR3$\ell$</a> <li><a href="?table=Cutflow%20Table">Cutflow Table</a> </ul> <b>Acceptances and Efficiencies:</b> <ul display="inline-block"> <li><a href="?table=Acceptance%20in%20the%20SRFR%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Acceptance in the SRFR region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Acceptance%20in%20the%20SRFR%20region%20with%20$\ell=$$e$">Acceptance in the SRFR region with $\ell=$$e$</a> <li><a href="?table=Acceptance%20in%20the%20SRFR%20region%20with%20$\ell=$$\mu$">Acceptance in the SRFR region with $\ell=$$\mu$</a> <li><a href="?table=Acceptance%20in%20the%20SRFR%20region%20with%20$\ell=$$\tau$">Acceptance in the SRFR region with $\ell=$$\tau$</a> <li><a href="?table=Acceptance%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Acceptance in the SR4$\ell$ region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Acceptance%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$e$">Acceptance in the SR4$\ell$ region with $\ell=$$e$</a> <li><a href="?table=Acceptance%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$\mu$">Acceptance in the SR4$\ell$ region with $\ell=$$\mu$</a> <li><a href="?table=Acceptance%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$\tau$">Acceptance in the SR4$\ell$ region with $\ell=$$\tau$</a> <li><a href="?table=Acceptance%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Acceptance in the SR3$\ell$ region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Acceptance%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$e$">Acceptance in the SR3$\ell$ region with $\ell=$$e$</a> <li><a href="?table=Acceptance%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$\mu$">Acceptance in the SR3$\ell$ region with $\ell=$$\mu$</a> <li><a href="?table=Acceptance%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$\tau$">Acceptance in the SR3$\ell$ region with $\ell=$$\tau$</a> <li><a href="?table=Efficiency%20in%20the%20SRFR%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Efficiency in the SRFR region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Efficiency%20in%20the%20SRFR%20region%20with%20$\ell=$$e$">Efficiency in the SRFR region with $\ell=$$e$</a> <li><a href="?table=Efficiency%20in%20the%20SRFR%20region%20with%20$\ell=$$\mu$">Efficiency in the SRFR region with $\ell=$$\mu$</a> <li><a href="?table=Efficiency%20in%20the%20SRFR%20region%20with%20$\ell=$$\tau$">Efficiency in the SRFR region with $\ell=$$\tau$</a> <li><a href="?table=Efficiency%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Efficiency in the SR4$\ell$ region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Efficiency%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$e$">Efficiency in the SR4$\ell$ region with $\ell=$$e$</a> <li><a href="?table=Efficiency%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$\mu$">Efficiency in the SR4$\ell$ region with $\ell=$$\mu$</a> <li><a href="?table=Efficiency%20in%20the%20SR4$\ell$%20region%20with%20$\ell=$$\tau$">Efficiency in the SR4$\ell$ region with $\ell=$$\tau$</a> <li><a href="?table=Efficiency%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$(e,%20\mu,%20\tau)$">Efficiency in the SR3$\ell$ region with $\ell=$$(e, \mu, \tau)$</a> <li><a href="?table=Efficiency%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$e$">Efficiency in the SR3$\ell$ region with $\ell=$$e$</a> <li><a href="?table=Efficiency%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$\mu$">Efficiency in the SR3$\ell$ region with $\ell=$$\mu$</a> <li><a href="?table=Efficiency%20in%20the%20SR3$\ell$%20region%20with%20$\ell=$$\tau$">Efficiency in the SR3$\ell$ region with $\ell=$$\tau$</a> <li><a href="?table=Triangle,%20Acceptance%20in%20SRFR,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Acceptance in SRFR, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Triangle,%20Acceptance%20in%20SR4$\ell$,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Acceptance in SR4$\ell$, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Triangle,%20Acceptance%20in%20SR3$\ell$,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Acceptance in SR3$\ell$, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Triangle,%20Efficiency%20in%20SRFR,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Efficiency in SRFR, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Triangle,%20Efficiency%20in%20SR4$\ell$,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Efficiency in SR4$\ell$, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Triangle,%20Efficiency%20in%20SR3$\ell$,%20$\ell=(e,%20\mu,%20\tau)$">Triangle, Efficiency in SR3$\ell$, $\ell=(e, \mu, \tau)$</a> <li><a href="?table=Acceptance%20by%20Final%20State%20in%20SRFR">Acceptance by Final State in SRFR</a> <li><a href="?table=Acceptance%20by%20Final%20State%20in%20SR4$\ell$">Acceptance by Final State in SR4$\ell$</a> <li><a href="?table=Acceptance%20by%20Final%20State%20in%20SR3$\ell$">Acceptance by Final State in SR3$\ell$</a> </ul>
The observed data and the SM background expectation in the CRs (pre-fit) and VRs (post-fit). The ''Other'' category mostly consists of tW Z, ttW, and tZ processes. The hatched bands indicate the combined theoretical, experimental, and MC statistical uncertainties. The bottom panel shows the fractional difference between the observed data and expected yields for the CRs and the significance of the difference for the VRs, computed following the profile likelihood method described in Ref. [arXiv: physics/0702156].
The observed yields and post-fit background expectations in SRFR, SR4$\ell$, and SR3$\ell$, shown inclusively and when the direct lepton from a $\tilde\chi^{\pm}_{1}/\tilde\chi^{0}_{1}$ decay is required to be an electron or muon. The Other category mostly consists of $tWZ$, $t\bar{t}W$, and $tZ$ processes. Uncertainties on the background expectation include combined statistical and systematic uncertainties. The individual uncertainties may be correlated and do not necessarily add in quadrature to equal the total background uncertainty.
A search for charged Higgs bosons decaying into a top quark and a bottom quark is presented. The data analysed correspond to 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$=13TeV, recorded with the ATLAS detector at the LHC. The production of a heavy charged Higgs boson in association with a top quark and a bottom quark, $pp\rightarrow tbH^{+}\rightarrow tbtb$, is explored in the $H^+$ mass range from 200 to 2000 GeV using final states with jets and one electron or muon. Events are categorised according to the multiplicity of jets and $b$-tagged jets, and multivariate analysis techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass; they range from 3.6 pb at 200 GeV to 0.036 pb at 2000 GeV at 95% confidence level. The results are interpreted in the hMSSM and $M_h^{125}$ scenarios.
Observed and expected upper limits for the production of $H^+\rightarrow tb$ in association with a top quark and a bottom quark. The bands surrounding the expected limit show the 68% and 95% confidence intervals. The red lines show the observed and expected 95% CL exclusion limits obtained with the 36 fb$^{-1}$ data sample. Theory predictions are shown for two representative values of $\tan\beta$ in the hMSSM benchmark scenario. Uncertainties in the predicted $H^+$ cross-sections or branching ratios are not considered.
Observed and expected limits on $\tan\beta$ as a function of $m_{H^+}$ in the hMSSM scenario. Limits are shown for $\tan\beta$ values in the range of 0.5-60 due to the availability of the model prediction. The bands surrounding the expected limits show the 68% and 95% confidence intervals. Uncertainties in the predicted $H^+$ cross-sections or branching ratios are not considered.
Observed and expected limits on $\tan\beta$ as a function of $m_{H^+}$ in the $M_h^{125}$ scenario. Limits are shown for $\tan\beta$ values in the range of 0.5-60 due to the availability of the model prediction. The bands surrounding the expected limits show the 68% and 95% confidence intervals. Uncertainties in the predicted $H^+$ cross-sections or branching ratios are not considered.
This paper presents studies of Bose-Einstein correlations (BEC) in proton-proton collisions at a centre-of-mass energy of 13 TeV, using data from the ATLAS detector at the CERN Large Hadron Collider. Data were collected in a special low-luminosity configuration with a minimum-bias trigger and a high-multiplicity track trigger, accumulating integrated luminosities of 151 $\mu$b$^{-1}$ and 8.4 nb$^{-1}$ respectively. The BEC are measured for pairs of like-sign charged particles, each with $|\eta|$ < 2.5, for two kinematic ranges: the first with particle $p_T$ > 100 MeV and the second with particle $p_T$ > 500 MeV. The BEC parameters, characterizing the source radius and particle correlation strength, are investigated as functions of charged-particle multiplicity (up to 300) and average transverse momentum of the pair (up to 1.5 GeV). The double-differential dependence on charged-particle multiplicity and average transverse momentum of the pair is also studied. The BEC radius is found to be independent of the charged-particle multiplicity for high charged-particle multiplicity (above 100), confirming a previous observation at lower energy. This saturation occurs independent of the transverse momentum of the pair.
Comparison of single-ratio two-particle correlation functions, C<sub>2</sub><sup>data</sup>(Q) and C<sub>2</sub><sup>MC</sup>(Q), with the two-particle double-ratio correlation function, R<sub>2</sub>(Q), for the high-multiplicity track (HMT) events using the opposite hemisphere (OHP) like-charge particles pairs reference sample for k<sub>T</sub> - interval 1000 < k<sub>T</sub> ≤ 1500 MeV.
Comparison of single-ratio two-particle correlation functions, C<sub>2</sub><sup>data</sup>(Q) and C<sub>2</sub><sup>MC</sup>(Q), with the two-particle double-ratio correlation function, R<sub>2</sub>(Q), for the high-multiplicity track (HMT) events using the unlike-charge particle (UCP) pairs reference sample for k<sub>T</sub> - interval 1000 < k<sub>T</sub> ≤ 1500 MeV.
The Bose-Einstein correlation (BEC) parameter R as a function of n<sub>ch</sub> for MB events using different MC generators in the calculation of R<sub>2</sub>(Q). The uncertainties shown are statistical. The lower panel of each plot shows the ratio of the BEC parameters obtained using EPOS LHC (red circles), Pythia 8 Monash (blue squares) and Herwig++ UE-EE-5 (green triangles) compared with the parameters obtained using Pythia 8 A2. The gray band in the lower panels is the MC systematic uncertainty, obtained as explained in the text.
A combination of measurements of the inclusive top-quark pair production cross-section performed by ATLAS and CMS in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV at the LHC is presented. The cross-sections are obtained using top-quark pair decays with an opposite-charge electron-muon pair in the final state and with data corresponding to an integrated luminosity of about 5 fb$^{-1}$ at $\sqrt{s}=7$ TeV and about 20 fb$^{-1}$ at $\sqrt{s}=8$ TeV for each experiment. The combined cross-sections are determined to be $178.5 \pm 4.7$ pb at $\sqrt{s}=7$ TeV and $243.3^{+6.0}_{-5.9}$ pb at $\sqrt{s}=8$ TeV with a correlation of 0.41, using a reference top-quark mass value of 172.5 GeV. The ratio of the combined cross-sections is determined to be $R_{8/7}= 1.363\pm 0.032$. The combined measured cross-sections and their ratio agree well with theory calculations using several parton distribution function (PDF) sets. The values of the top-quark pole mass (with the strong coupling fixed at 0.118) and the strong coupling (with the top-quark pole mass fixed at 172.5 GeV) are extracted from the combined results by fitting a next-to-next-to-leading-order plus next-to-next-to-leading-log QCD prediction to the measurements. Using a version of the NNPDF3.1 PDF set containing no top-quark measurements, the results obtained are $m_t^\text{pole} = 173.4^{+1.8}_{-2.0}$ GeV and $\alpha_\text{s}(m_Z)= 0.1170^{+ 0.0021}_{-0.0018}$.
Full covariance matrix including all systematic uncertainties expressed as nuisance parameters. With the exception of the cross section parameters, all parameters were normalised to 1 before the fit. Therefore, the diagonal elements represent the constraint in quadrature.
Full covariance matrix including all systematic uncertainties expressed as nuisance parameters. With the exception of the cross section parameters, all parameters were normalised to 1 before the fit. Therefore, the diagonal elements represent the constraint in quadrature.
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a $\tau$-lepton is presented. The search is based on a dataset of $pp$ collisions at $\sqrt{s}=13$ TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying $\tau$-lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing $b$-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying $\tau$-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into $t\tau$ and $b\nu$. Scalar leptoquarks decaying exclusively into $t\tau$ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into $t\tau$, the lower mass limit is 1.22 TeV.
Selection efficiency times acceptance summed over the seven signal regions as a function of $m_{\mathrm{LQ}_{3}^{\mathrm{d}}}$, assuming B = 1.
Summary of the observed and expected 95% CL upper limits on the cross section for $\mathrm{LQ}_{3}^{\mathrm{d}}$ pair production as a function of $m_{\mathrm{LQ}_{3}^{\mathrm{d}}}$ under the assumptions of B=1.
Summary of the observed and expected 95% CL upper limits on B as a function of $m_{\mathrm{LQ}_{3}^{\mathrm{d}}}$.
Searches for new resonances in the diphoton final state, with spin 0 as predicted by theories with an extended Higgs sector and with spin 2 using a warped extra-dimension benchmark model, are presented using 139 fb$^{-1}$ of $\sqrt{s} = $ 13 TeV $pp$ collision data collected by the ATLAS experiment at the LHC. No significant deviation from the Standard Model is observed and upper limits are placed on the production cross-section times branching ratio to two photons as a function of the resonance mass.
The expected and observed upper limits at 95\% CL on the fiducial cross-section times branching ratio to two photons of a narrow-width (Γ_X = 4 MeV) spin-0 resonance as a function of its mass m_X. For masses greater than 1000 GeV, pseudo-experiments are used to verify the expected and observed limits, and used in place of the asymptotic limit when differences are observed.
The expected and observed upper limits at 95\% CL on the production cross-section times branching ratio to two photons of the lightest KK graviton as a function of its mass for k/Mpl=0.10. For masses greater than 1000 GeV, pseudo-experiments are used to verify the expected and observed limits, and used in place of the asymptotic limit when differences are observed.
Expected and observed limits computed using asymptotic formulas as a function of the signal mass m_{X} and the relative width $\Gamma_{X}/m_{X}$ for the spin-0 resonance search.
Electroweak symmetry breaking explains the origin of the masses of elementary particles through their interactions with the Higgs field. Besides the measurements of the Higgs boson properties, the study of the scattering of massive vector bosons with spin one allows the nature of electroweak symmetry breaking to be probed. Among all processes related to vector-boson scattering, the electroweak production of two jets and a $Z$-boson pair is a rare and important one. Here we report the observation of this process from proton-proton collision data corresponding to an integrated luminosity of 139/fb recorded at a centre-of-mass energy of 13 TeV with the ATLAS detector at the Large Hadron Collider. We consider two different final states originating from the decays of the $Z$-boson pair - one containing four charged leptons and the other containing two charged leptons and two neutrinos. The hypothesis of no electroweak production is rejected with a statistical significance of 5.7 $\sigma$, and the measured cross-section for electroweak production is consistent with the standard model prediction. In addition, we report cross-sections for inclusive production of a $Z$-boson pair and two jets for the two final states.
Signal strength and significance of EW ZZjj processes
Measured and predicted fiducial cross-sections in both the lllljj and ll$\nu\nu$jj channels for the inclusive ZZjj processes. Uncertainties due to different sources are presented.
Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ QCD CR.
Inclusive and differential measurements of the top-antitop ($t\bar{t}$) charge asymmetry $A_\text{C}^{t\bar{t}}$ and the leptonic asymmetry $A_\text{C}^{\ell\bar{\ell}}$ are presented in proton-proton collisions at $\sqrt{s} = 13$ TeV recorded by the ATLAS experiment at the CERN Large Hadron Collider. The measurement uses the complete Run 2 dataset, corresponding to an integrated luminosity of 139 fb$^{-1}$, combines data in the single-lepton and dilepton channels, and employs reconstruction techniques adapted to both the resolved and boosted topologies. A Bayesian unfolding procedure is performed to correct for detector resolution and acceptance effects. The combined inclusive $t\bar{t}$ charge asymmetry is measured to be $A_\text{C}^{t\bar{t}} = 0.0068 \pm 0.0015$, which differs from zero by 4.7 standard deviations. Differential measurements are performed as a function of the invariant mass, transverse momentum and longitudinal boost of the $t\bar{t}$ system. Both the inclusive and differential measurements are found to be compatible with the Standard Model predictions, at next-to-next-to-leading order in quantum chromodynamics perturbation theory with next-to-leading-order electroweak corrections. The measurements are interpreted in the framework of the Standard Model effective field theory, placing competitive bounds on several Wilson coefficients.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Results:</b> <ul> <li><a href="132116?version=2&table=Resultsforchargeasymmetryinclusive">$A_C^{t\bar{t}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvsmtt">$A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvspttt">$A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvsbetatt">$A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$</a> <li><a href="132116?version=2&table=Resultsforleptonicchargeasymmetryinclusive">$A_C^{\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvsllmll">$A_C^{\ell\bar{\ell}}$ vs $m_{\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvsllptll">$A_C^{\ell\bar{\ell}}$ vs $p_{T,\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=Resultsforchargeasymmetryvsllbetall">$A_C^{\ell\bar{\ell}}$ vs $\beta_{z,\ell\bar{\ell}}$</a> </ul> <b>Bounds on the Wilson coefficients:</b> <ul> <li><a href="132116?version=2&table=BoundsonWilsoncoefficientschargeasymmetryinclusive">$A_C^{t\bar{t}}$</a> <li><a href="132116?version=2&table=BoundsonWilsoncoefficientschargeasymmetryvsmtt">$A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$</a> </ul> <b>Ranking of systematic uncertainties:</b></br> Inclusive:<a href="132116?version=2&table=NPrankingchargeasymmetryinclusive">$A_C^{t\bar{t}}$</a></br> <b>$A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$:</b> <ul> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsbetattbin0">$\beta_{z,t\bar{t}} \in[0,0.3]$</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsbetattbin1">$\beta_{z,t\bar{t}} \in[0.3,0.6]$</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsbetattbin2">$\beta_{z,t\bar{t}} \in[0.6,0.8]$</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsbetattbin3">$\beta_{z,t\bar{t}} \in[0.8,1]$</a> </ul> <b>$A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$:</b> <ul> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsmttbin0">$m_{t\bar{t}}$ < $500$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsmttbin1">$m_{t\bar{t}} \in [500,750]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsmttbin2">$m_{t\bar{t}} \in [750,1000]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsmttbin3">$m_{t\bar{t}} \in [1000,1500]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsmttbin4">$m_{t\bar{t}}$ > $1500$GeV</a> </ul> <b>$A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$:</b> <ul> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsptttbin0">$p_{T,t\bar{t}} \in [0,30]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsptttbin1">$p_{T,t\bar{t}} \in[30,120]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsptttbin2">$p_{T,t\bar{t}}$ > $120$GeV</a> </ul> Inclusive leptonic:<a href="132116?version=2&table=NPrankingleptonicchargeasymmetryinclusive">$A_C^{\ell\bar{\ell}}$</a></br> <b>$A_C^{\ell\bar{\ell}}$ vs $\beta_{z,\ell\bar{\ell}}$</b> <ul> <li><a href="132116?version=2&tableNPrankingchargeasymmetry=vsllbetallbin0">$\beta_{z,\ell\bar{\ell}} \in [0,0.3]$</a> <li><a href="132116?version=2&tableNPrankingchargeasymmetry=vsllbetallbin1">$\beta_{z,\ell\bar{\ell}} \in [0.3,0.6]$</a> <li><a href="132116?version=2&tableNPrankingchargeasymmetry=vsllbetallbin2">$\beta_{z,\ell\bar{\ell}} \in [0.6,0.8]$</a> <li><a href="132116?version=2&tableNPrankingchargeasymmetry=vsllbetallbin3">$\beta_{z,\ell\bar{\ell}} \in [0.8,1]$</a> </ul> <b>$A_C^{\ell\bar{\ell}}$ vs $m_{\ell\bar{\ell}}$</b> <ul> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllmllbin0">$m_{\ell\bar{\ell}}$ < $200$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllmllbin1">$m_{\ell\bar{\ell}} \in [200,300]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllmllbin2">$m_{\ell\bar{\ell}} \in [300,400]$Ge$</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllmllbin3">$m_{\ell\bar{\ell}}$ > $400$GeV</a> </ul> <b>$A_C^{\ell\bar{\ell}}$ vs $p_{T,\ell\bar{\ell}}$</b> <ul> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllptllbin0">$p_{T,\ell\bar{\ell}}\in [0,20]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllptllbin1">$p_{T,\ell\bar{\ell}}\in[20,70]$GeV</a> <li><a href="132116?version=2&table=NPrankingchargeasymmetryvsllptllbin2">$p_{T,\ell\bar{\ell}}$ > $70$GeV</a> </ul> <b>NP correlations:</b> <ul> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryinclusive">$A_C^{t\bar{t}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvsmtt">$A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvspttt">$A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvsbetatt">$A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$</a> <li><a href="132116?version=2&table=NPcorrelationsleptonicchargeasymmetryinclusive">$A_c^{\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvsllmll">$A_c^{\ell\bar{\ell}}$ vs $m_{\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvsllptll">$A_C^{\ell\bar{\ell}}$ vs $p_{T,\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=NPcorrelationschargeasymmetryvsllbetall">$A_C^{\ell\bar{\ell}}$ vs $\beta_{z,\ell\bar{\ell}}$</a> </ul> <b>Covariance matrices:</b> <ul> <li><a href="132116?version=2&table=Covariancematrixchargeasymmetryvsmtt">$A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$</a> <li><a href="132116?version=2&table=Covariancematrixchargeasymmetryvspttt">$A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$</a> <li><a href="132116?version=2&table=Covariancematrixchargeasymmetryvsbetatt">$A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$</a> <li><a href="132116?version=2&table=Covariancematrixleptonicchargeasymmetryvsllmll">$A_c^{\ell\bar{\ell}}$ vs $m_{\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=Covariancematrixleptonicchargeasymmetryvsllptll">$A_C^{\ell\bar{\ell}}$ vs $p_{T,\ell\bar{\ell}}$</a> <li><a href="132116?version=2&table=Covariancematrixleptonicchargeasymmetryvsllbetall">$A_C^{\ell\bar{\ell}}$ vs $\beta_{z,\ell\bar{\ell}}$</a> </ul>
The unfolded inclusive charge asymmetry. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed, and the impact of the linear term of the Wilson coefficient on the $A_C^{t\bar{t}}$ prediction is shown for two different values. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.
The unfolded differential charge asymmetry as a function of the invariant mass of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed, and the impact of the linear term of the Wilson coefficient on the $A_C^{t\bar{t}}$ prediction is shown for two different values. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.
A search for quantum black holes in electron+jet and muon+jet invariant mass spectra is performed with 140 fb$^{-1}$ of data collected by the ATLAS detector in proton-proton collisions at $\sqrt{s}$ = 13 TeV at the Large Hadron Collider. The observed invariant mass spectrum of lepton+jet pairs is consistent with Standard Model expectations. Upper limits are set at 95% confidence level on the production cross-sections times branching fractions for quantum black holes decaying into a lepton and a quark in a search region with invariant mass above 2.0 TeV. The resulting quantum black hole lower mass threshold limit is 9.2 TeV in the Arkani-Hamed-Dimopoulos-Dvali model, and 6.8 TeV in the Randall-Sundrum model.
The 95% CL model-independent upper limits on $\sigma \times Br$ for the non-SM signal production with decay into the lepton+jet. The limits take into account statistical and systematic uncertainties. Circles along the solid red line indicate the lower border of the SR (threshold of SR, Th$_\mathrm{SR}$), above which the observed limit is computed. The expected limits are shown by the dashed line. The $\pm 1\sigma$ and $\pm 2\sigma$ bands of expected limits are shown in green and yellow, respectively. The limits are obtained with pseudo-experiments.
The combined 95% CL upper limits on $\sigma \times Br$ as a function of threshold mass, $M_\mathrm{th}$, for QBH production with decay into lepton+jet for ADD-model (extra dimensions n = 6). The limits take into account statistical and systematic uncertainties. Circles along the solid red line indicate the mass $M_\mathrm{th}$ of the signal where the observed limit is computed. The expected limits are shown by the dashed line. The $\pm 1\sigma$ and $\pm 2\sigma$ bands are shown in green and yellow, respectively. The theoretically predicted $\sigma \times Br$ for the QBH production and decay is shown as the solid blue curve with squares.
The combined 95% CL upper limits on $\sigma \times Br$ as a function of threshold mass, $M_\mathrm{th}$, for QBH production with decay into lepton+jet for RS1-model (extra dimensions n = 1). The limits take into account statistical and systematic uncertainties. Circles along the solid red line indicate the mass $M_\mathrm{th}$ of the signal where the observed limit is computed. The expected limits are shown by the dashed line. The $\pm 1\sigma$ and $\pm 2\sigma$ bands are shown in green and yellow, respectively. The theoretically predicted $\sigma \times Br$ for the QBH production and decay is shown as the solid blue curve with squares.
Measurements of the suppression and correlations of dijets is performed using 3 $\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$ TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32 GeV to 398 GeV and the centrality of the collisions. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurements at $\sqrt{s_{\mathrm{NN}}} =5.02$ TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear-modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference between the center-of-mass energies of the initial parton scattering process in Xe+Xe and Pb+Pb collisions. These results should provide input for a better understanding of the role of energy density, system size, path length, and fluctuations in the parton energy loss.
The centrality intervals in Xe+Xe collisions and their corresponding TAA with absolute uncertainties.
The centrality intervals in Xe+Xe and Pb+Pb collisions for matching SUM ET FCAL intervals and respective TAA values for Xe+Xe collisions.
The performance of the jet energy scale (JES) for jets with $|y| < 2.1$ evaluated as a function of pT_truth in different centrality bins. Simulated hard scatter events were overlaid onto events from a dedicated sample of minimum-bias Xe+Xe data.
A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the Standard Model $Z$ boson is presented, using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark Higgs boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon's coupling to the dark Higgs boson times the kinetic mixing between the Standard Model photon and the dark photon, $\alpha_{D}\varepsilon^2$, in the dark photon mass range of $[5, 40]$ GeV except for the $\Upsilon$ mass window $[8.8, 11.1]$ GeV. This search explores new parameter space not previously excluded by other experiments.
Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 20 GeV
Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 30 GeV
Observed and expected upper limits at 95% CL on the production cross-section times branching fraction as a function of $m_{A'}$ at dark Higgs boson mass of 40 GeV
A search for a new pseudoscalar $a$-boson produced in events with a top-quark pair, where the $a$-boson decays into a pair of muons, is performed using $\sqrt{s} = 13$ TeV $pp$ collision data collected with the ATLAS detector at the LHC, corresponding to an integrated luminosity of $139\, \mathrm{fb}^{-1}$. The search targets the final state where only one top quark decays to an electron or muon, resulting in a signature with three leptons $e\mu\mu$ and $\mu\mu\mu$. No significant excess of events above the Standard Model expectation is observed and upper limits are set on two signal models: $pp \rightarrow t\bar{t}a$ and $pp \rightarrow t\bar{t}$ with $t \rightarrow H^\pm b$, $H^\pm \rightarrow W^\pm a$, where $a\rightarrow\mu\mu$, in the mass ranges $15$ GeV $ < m_a < 72$ GeV and $120$ GeV $ \leq m_{H^{\pm}} \leq 160$ GeV.
Comparison between data and expected background for the on-$Z$-boson control region in the $e\mu\mu$ final state. The bins correspond to different jet and $b$-jet multiplicities. Rare background processes include $ZZ+$jets, $WWZ$, $WZZ$, $ZZZ$, and $t\bar{t}t\bar{t}$.
Comparison between data and expected background for the on-$Z$boson control region in the $\mu\mu\mu$ final state. The bins correspond to different jet and $b$-jet multiplicities. Rare background processes include $ZZ+$jets, $WWZ$, $WZZ$, $ZZZ$, and $t\bar{t}t\bar{t}$.
Di-muon mass distribution for the $e\mu\mu$ signal region for data and expected background. The expected signal distribution for $m_a = 35$ GeV is shown assuming $\sigma(t\bar{t}a)\times \text{Br}(a\rightarrow\mu\mu) = 4$ fb. Rare background processes include $ZZ+$jets, $WWZ$, $WZZ$, $ZZZ$, and $t\bar{t}t\bar{t}$.
This Letter reports the observation of $WZ\gamma$ production and a measurement of its cross-section using 140.1 $\pm$ 1.2 fb$^{-1}$ of proton-proton collision data recorded at a center-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The $WZ\gamma$ production cross-section, with both the $W$ and $Z$ bosons decaying leptonically, $pp \rightarrow WZ\gamma \rightarrow {\ell'}^{\pm}\nu\ell^{+}\ell^{-}\gamma$ ($\ell^{(')} = e, \mu$), is measured in a fiducial phase-space region defined such that the leptons and the photon have high transverse momentum and the photon is isolated. The cross-section is found to be 2.01 $\pm$ 0.30 (stat.) $\pm$ 0.16 (syst) fb. The corresponding Standard Model predicted cross-section calculated at next-to-leading order in perturbative quantum chromodynamics and at leading order in the electroweak coupling constant is 1.50 $\pm$ 0.06 fb. The observed significance of the $WZ\gamma$ signal is 6.3$\sigma$, compared with an expected significance of 5.0$\sigma$.
Events in bins of the photon $p_{\mathrm{T}}^{\gamma}$ in the SR.
Events in bins of the $p_{\mathrm{T}}^{\ell_{1}}$ in the SR.
Events in bins of the $m(\ell\ell)$ in the SR.
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.
The post-fit yields in the nine bins of the $(p_\textrm{T}^{\textrm{bal}}, |\phi_{\textrm{max}} - \phi_{\textrm{min}}|)$ grid. Error band includes all the systematic uncertainties.
The post-fit distributions of HT for the SR. Data are compared with background predictions, and six signal predictions covering a representative mediator mass and invisible fraction range are overlaid. The uncertainties include all systematic and statistical components. The last bin contains the overflow.
The post-fit distributions of $E_{\text{T}}^{\text{miss}}$ for the SR. Data are compared with background predictions, and six signal predictions covering a representative mediator mass and invisible fraction range are overlaid. The uncertainties include all systematic and statistical components. The last bin contains the overflow.
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 measurement of hard scatterings in proton-nucleus collisions has resulted in a greater understanding of both the proton and nuclear structure. ATLAS measured the centrality dependence of the dijet yield using 165 nb$^{-1}$ of $p$+Pb data collected at $\sqrt{s_{_\text{NN}}}$ = 8.16 TeV in 2016. The event centrality, which reflects the $p$+Pb impact parameter, is characterized by the total transverse energy registered in the Pb-going side of the forward calorimeter. The central-to-peripheral ratio of the scaled dijet yields, $R_\mathrm{CP}$, is evaluated, and the results are presented as a function of variables that reflect the kinematics of the initial hard parton scattering process. The $R_\mathrm{CP}$ shows a scaling with the Bjorken-$x$ of the parton originating from the proton, $x_p$, while no such trend is observed as a function of $x_\mathrm{Pb}$. This analysis provides unique input to understanding the role of small proton spatial configurations in $p$+Pb collisions by covering parton momentum fractions from the valence region down to $x_p \sim 10^{-3}$ and $x_\mathrm{Pb}\sim 4\cdot10^{-4}$.
$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-3.0 < y_b < -2.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.
$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-2.0 < y_b < -1.0$ and $0.0 < y^* < 1.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.
$R_\text{CP}$ plotted as a function of approximated $x_p$ for $-2.0 < y_b < -1.0$ and $1.0 < y^* < 2.0$, constructed using $\langle y_{\text{b}} \rangle$ and $\langle y^{*} \rangle$. The proton-going direction is defined by $y_{\text{b}} > 0$.
Measurements of the substructure of top-quark jets are presented, using 140 fb$^{-1}$ of 13 TeV $pp$ collision data recorded with the ATLAS detector at the LHC. Top-quark jets reconstructed with the anti-$k_{t}$ algorithm with a radius parameter $R=1.0$ are selected in top-quark pair ($t\bar{t}$) events where one top quark decays semileptonically and the other hadronically, or where both top quarks decay hadronically. The top-quark jets are required to have transverse momentum $p_\mathrm{T} > 350$ GeV, yielding large samples of data events with jet $p_\mathrm{T}$ values between 350 and 600 GeV. One- and two-dimensional differential cross-sections for eight substructure variables, defined using only the charged components of the jets, are measured in a particle-level phase space by correcting for the smearing and acceptance effects induced by the detector. The differential cross-sections are compared with the predictions of several Monte Carlo simulations in which top-quark pair-production quantum chromodynamic matrix-element calculations at next-to-leading-order precision in the strong coupling constant $\alpha_\mathrm{S}$ are passed to leading-order parton shower and hadronization generators. The Monte Carlo predictions for measures of the broadness, and also the two-body structure, of the top-quark jets are found to be in good agreement with the measurements, while variables sensitive to the three-body structure of the top-quark jets exhibit some tension with the measured distributions.
Absolute differential cross-section as a function of RC large-R jet $\tau_{32}$ at particle level in the $\ell$+jets channel. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the Absolute differential cross-section as function of RC large-R jet $\tau_{32}$ at particle level in the $\ell$+jets channel, accounting for the statistical uncertainty.
Relative differential cross-section as a function of RC large-R jet $\tau_{32}$ at particle level in the $\ell$+jets channel. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Results from a wide range of searches targeting different experimental signatures with and without missing transverse momentum ($E_{\mathrm{T}}^{\mathrm{miss}}$) are used to constrain a Two-Higgs-Doublet Model (2HDM) with an additional pseudo-scalar mediating the interaction between ordinary and dark matter (2HDM+$a$). The analyses use up to 139 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy $\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider during 2015-2018. The results from three of the most sensitive searches are combined statistically. These searches target signatures with large $E_{\mathrm{T}}^{\mathrm{miss}}$ and a leptonically decaying $Z$ boson; large $E_{\mathrm{T}}^{\mathrm{miss}}$ and a Higgs boson decaying to bottom quarks; and production of charged Higgs bosons in final states with top and bottom quarks, respectively. Constraints are derived for several common and new benchmark scenarios in the 2HDM+$a$.
Observed combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
Expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
1 sigma band of expected combination limits at 95% CL in the $(m_{a},m_{A})$ plane under the assumption of $sin\theta$ = 0.35.
The inclusive top-quark-pair production cross section $\sigma_{t\bar{t}}$ and its ratio to the $Z$-boson production cross section have been measured in proton--proton collisions at $\sqrt{s} = 13.6$ TeV, using 29 fb${}^{-1}$ of data collected in 2022 with the ATLAS experiment at the Large Hadron Collider. Using events with an opposite-charge electron-muon pair and $b$-tagged jets, and assuming Standard Model decays, the top-quark-pair production cross section is measured to be $\sigma_{t\bar{t}} = 850 \pm 3\mathrm{(stat.)}\pm 18\mathrm{(syst.)}\pm 20\mathrm{(lumi.)}$ pb. The ratio of the $t\bar{t}$ and the $Z$-boson production cross sections is also measured, where the $Z$-boson contribution is determined for inclusive $e^+e^-$ and $\mu^+\mu^-$ events in a fiducial phase space. The relative uncertainty on the ratio is reduced compared to the $t\bar{t}$ cross section, thanks to the cancellation of several systematic uncertainties. The result for the ratio, $R_{t\bar{t}/Z} = 1.145 \pm 0.003\mathrm{(stat.)}\pm 0.021\mathrm{(syst.)}\pm 0.002\mathrm{(lumi.)}$ is consistent with the Standard Model prediction using the PDF4LHC21 PDF set.
The fiducial phase-space definition for the $Z$-boson measurement. Born-level leptons are used.
The measured $t\bar{t}$ cross section and the ratio of the cross sections of $t\bar{t}$ and the $Z$-boson. Full phase-space is considered for $t\bar{t}$, while fiducial phase-space is considered for the $Z$-boson.
Table with pre-fit yields in the four regions used in the measurement
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.
The main sources of systematic uncertainty for the $X\to Z \gamma$ search. The gluon-gluon fusion spin-0 signal samples produced at $m_{X} = [220-3400]$ GeV are used to evaluate the systematic uncertainty. The ranges for the uncertainties span the variations among different categories and different $m_{X}$ resonance masses. The uncertainty due to the spurious signal uncertainty is reported as the absolute number of events. In the table, "ID" for photon and electrons refers to identification efficiency uncertainties, "ISO" refers to isolation efficiency uncertainties, "TRIG" refers to trigger efficiency uncertainties, "RECO" refers to muon reconstruction efficiency uncertainty and "TTVA" refers to muon track-to-vertex-association efficiency uncertainty.
The observed (expected) upper limits of $\sigma(pp\to X)\cdot\mathcal{B}(X\to Z\gamma)$ for spin-0 and spin-2 heavy resonances at 95\% CL. $m_{X}$ varies from 220 GeV to 3400~\GeV.
Impacts of grouped dominant systematic uncertainties. The impact corresponds to the relative variation of the asymptotic expected upper limit of $\sigma(pp \rightarrow X) \times BR(X \rightarrow Z\gamma)$ from $m_{X}=220$ GeV to $m_{X}=3.4$ TeV when re-evaluating the quantity by fixing the corresponding nuisance parameters to the best-fit values, while keeping others free to float. The impact of total systematic uncertainties are performed in the last row.
This Letter presents the measurement of the fiducial and differential cross-sections of the electroweak production of a $Z \gamma$ pair in association with two jets. The analysis uses 140 fb$^{-1}$ of LHC proton-proton collision data taken at $\sqrt{s}$=13 TeV recorded by the ATLAS detector during the years 2015-2018. Events with a $Z$ boson candidate decaying into either an $e^+e^-$ or $\mu^+ \mu^-$ pair, a photon and two jets are selected. The electroweak component is extracted by requiring a large dijet invariant mass and a large rapidity gap between the two jets and is measured with an observed and expected significance well above five standard deviations. The fiducial $pp \rightarrow Z \gamma jj$ cross-section for the electroweak production is measured to be 3.6 $\pm$ 0.5 fb. The total fiducial cross-section that also includes contributions where the jets arise from strong interactions is measured to be $16.8^{+2.0}_{-1.8}$ fb. The results are consistent with the Standard Model predictions. Differential cross-sections are also measured using the same events and are compared with parton-shower Monte Carlo simulations. Good agreement is observed between data and predictions.
Post-fit mjj distributions in the mjj>500 GeV SR. The uncertainty band around the expectation includes all systematic uncertainties (including MC statistical uncertainty) and takes into account their correlations as obtained from the fit. The error bar around the data points represents the data statistical uncertainty. Events beyond the upper limit of the histogram are included in the last bin.
Post-fit mjj distributions in the mjj>500 GeV CR. The uncertainty band around the expectation includes all systematic uncertainties (including MC statistical uncertainty) and takes into account their correlations as obtained from the fit. The error bar around the data points represents the data statistical uncertainty. Events beyond the upper limit of the histogram are included in the last bin.
Post-fit mjj distributions in the mjj>150 GeV Extended SR. The uncertainty band around the expectation includes all systematic uncertainties (including MC statistical uncertainty) and takes into account their correlations as obtained from the fit. The error bar around the data points represents the data statistical uncertainty. Events beyond the upper limit of the histogram are included in the last bin.
New particles with large masses that decay into hadronically interacting particles are predicted by many models of physics beyond the Standard Model. A search for a massive resonance that decays into pairs of dijet resonances is performed using 140 fb$^{-1}$ of proton$-$proton collisions at $\sqrt{s}=13$ TeV recorded by the ATLAS detector during Run 2 of the Large Hadron Collider. Resonances are searched for in the invariant mass of the tetrajet system, and in the average invariant mass of the pair of dijet systems. A data-driven background estimate is obtained by fitting the tetrajet and dijet invariant mass distributions with a four-parameter dijet function and a search for local excesses from resonant production of dijet pairs is performed. No significant excess of events beyond the Standard Model expectation is observed, and upper limits are set on the production cross-sections of new physics scenarios.
The average tetrajet invariant mass distributions in data, along with the fitted background estimates for 0.10 < $\alpha$ < 0.12.
The average tetrajet invariant mass distributions in data, along with the fitted background estimates for 0.12 < $\alpha$ < 0.14.
The average tetrajet invariant mass distributions in data, along with the fitted background estimates for 0.14 < $\alpha$ < 0.16.
The first evidence for the Higgs boson decay to a $Z$ boson and a photon is presented, with a statistical significance of 3.4 standard deviations. The result is derived from a combined analysis of the searches performed by the ATLAS and CMS Collaborations with proton-proton collision data sets collected at the CERN Large Hadron Collider (LHC) from 2015 to 2018. These correspond to integrated luminosities of around 140 fb$^{-1}$ for each experiment, at a center-of-mass energy of 13 TeV. The measured signal yield is $2.2\pm0.7$ times the Standard Model prediction, and agrees with the theoretical expectation within 1.9 standard deviations.
The negative profile log-likelihood test statistic, where $\Lambda$ represents the likelihood ratio, as a function of the signal strength $\mu$ derived from the ATLAS data, the CMS data, and the combined result.
This letter reports the observation of $W(\ell\nu)\gamma\gamma$ production in proton-proton collisions. This measurement uses the full Run 2 sample of events recorded at a center-of-mass energy of $\sqrt{s} = 13$ TeV by the ATLAS detector at the LHC, corresponding to an integrated luminosity of 140 fb$^{-1}$. Events with a leptonically-decaying $W$ boson and at least two photons are considered. The background-only hypothesis is rejected with an observed and expected significance of $5.6$ standard deviations. The inclusive fiducial production cross section of $W(e\nu)\gamma\gamma$ and $W(\mu\nu)\gamma\gamma$ events is measured to be $\sigma_{\mathrm{fid}} = 13.8 \pm 1.1 (\mathrm{stat}) \substack{+2.1 \\ -2.0} (\mathrm{syst}) \pm 0.1 (\mathrm{lumi})$ fb, in agreement with the Standard Model prediction.
The measured fiducial $W(\rightarrow e\nu / \mu\nu)\gamma\gamma$ integrated cross section compared with both the signal event generator predictions.
A search is conducted for a new scalar boson $S$, with a mass distinct from that of the Higgs boson, decaying into four leptons ($\ell =$$e$, $\mu$) via an intermediate state containing two on-shell, promptly decaying new spin-1 bosons $Z_\text{d}$: $S \rightarrow Z_\text{d}Z_\text{d} \rightarrow 4\ell$, where the $Z_\text{d}$ boson has a mass between 15 and 300 GeV, and the $S$ boson has a mass between either 30 and 115 GeV or 130 and 800 GeV. The search uses proton-proton collision data collected with the ATLAS detector at the Large Hadron Collider with an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy of $\sqrt{s}=13$ TeV. No significant excess above the Standard Model background expectation is observed. Upper limits at 95% confidence level are set on the production cross-section times branching ratio, $\sigma(gg \to S) \times \mathcal{B}(S\rightarrow Z_\text{d}Z_\text{d} \rightarrow 4\ell)$, as a function of the mass of both particles, $m_S$ and $m_{Z\text{d}}$.
Average dilepton mass distribution $\left\langle m_{\ell\ell}\right\rangle = \frac{1}{2}\left(m_{ab} + m_{cd}\right)$ in Signal Region 1.
Average dilepton mass distribution $\left\langle m_{\ell\ell}\right\rangle = \frac{1}{2}\left(m_{ab} + m_{cd}\right)$ in Signal Region 2.
Total invariant mass distribution $m_{4\ell}$ in Signal Region 1.
A measurement of the invisible width of the $Z$ boson using events with jets and missing transverse momentum is presented using 37 $\mbox{fb\(^{-1}\)}$ of 13 TeV proton-proton data collected by the ATLAS detector in 2015 and 2016. The ratio of $Z\rightarrow \textrm{inv}$ to $Z\rightarrow\ell\ell$ events, where inv refers to non-detected particles and $\ell$ is either an electron or a muon, is measured and corrected for detector effects. Events with at least one energetic central jet with $p_{\textrm{T}} \geq 110$ GeV are selected for both the $Z\rightarrow \textrm{inv}$ and $Z\rightarrow\ell\ell$ final states to obtain a similar phase space in the ratio. The invisible width is measured to be $506\pm2 \textrm{ (stat.)} \pm12 \textrm{ (syst.)}$ MeV and is the single most precise recoil-based measurement. The result is in agreement with the most precise determination from LEP and the Standard Model prediction based on three neutrino generations.
Measured invisible width of the $Z$ boson, $\Gamma(Z\rightarrow \textrm{inv})$.
Measured $\mathrm{R}^{\mathrm{miss}}_{ee}$.
Measured $\mathrm{R}^{\mathrm{miss}}_{\mu\mu}$.
A search for the decay of the Higgs boson to a $Z$ boson and a light, pseudoscalar particle, $a$, decaying respectively to two leptons and to two photons is reported. The search uses the full LHC Run 2 proton-proton collision data at $\sqrt{s}=13$ TeV, corresponding to 139 fb$^{-1}$ collected by the ATLAS detector. This is one of the first searches for this specific decay mode of the Higgs boson, and it probes unexplored parameter space in models with axion-like particles (ALPs) and extended scalar sectors. The mass of the $a$ particle is assumed to be in the range 0.1-33 GeV. The data are analysed in two categories: a merged category where the photons from the $a$ decay are reconstructed in the ATLAS calorimeter as a single cluster, and a resolved category in which two separate photons are detected. The main background processes are from Standard Model $Z$ boson production in association with photons or jets. The data are in agreement with the background predictions, and upper limits on the branching ratio of the Higgs boson decay to $Za$ times the branching ratio $a\to\gamma\gamma$ are derived at the 95% confidence level and they range from 0.08% to 2% depending on the mass of the $a$ particle. The results are also interpreted in the context of ALP models.
Post-fit distribution for $m_{\gamma\gamma}$ for the resolved category in number of events per 0.2 GeV for data. The figure uses $pp$ collision data at $\sqrt{s}=13$ TeV corresponding to 139 fb$^{-1}$.
Post-fit distribution for $m_{\gamma\gamma}$ for the resolved category in number of events per 0.2 GeV for a signal distribution for $m_a = 9$ GeV, and the signal plus background fit with its background component. The branching ratio of the Higgs boson decay to $Za$ times the branching ratio $a $->$ \gamma \gamma$ is assumed to be 50%. The figure uses $pp$ collision data at $\sqrt{s}=13$ TeV corresponding to 139 fb$^{-1}$.
Post-fit final discriminating variable $\Delta R_{Z\gamma}$ in the signal region of the merged category. Signal distributions for $m_a$ values used in this category are overlayed for comparison, assuming a branching ratio of the Higgs boson decay to $Za$ times the branching ratio $a $->$ \gamma \gamma$ of 100%. The signal yields have been multiplied by 10 for better visibility. The figure uses $pp$ collision data at $\sqrt{s}=13$ TeV corresponding to 139 fb$^{-1}$.
The associated production of Higgs and $W$ bosons via vector-boson fusion (VBF) is highly sensitive to the relative sign of the Higgs boson couplings to $W$ and $Z$ bosons. In this Letter, two searches for this process are presented, using 140 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC. The first search targets scenarios with opposite-sign couplings of the $W$ and $Z$ bosons to the Higgs boson, while the second targets Standard Model-like scenarios with same-sign couplings. Both analyses consider Higgs decays into a pair of $b$-quarks and $W$ decays with an electron or muon. The opposite-sign coupling hypothesis is excluded with significance much greater than $5\sigma$, and the observed (expected) upper limit set on the cross-section for VBF $WH$ production is 9.0 (8.7) times the Standard Model value.
Data compared to the background prediction in each region of the negative $\lambda_{WZ}$ analysis, before the fit to data. The signal prediction with $\kappa_{W} = +1$, $\kappa_{Z} = -1$ is shown overlaid. The predicted signal yield with $\kappa_{W} = +1$, $\kappa_{Z} = +1$ in SR$^{-}$ is 2.93 events, which is not shown in the figure. The shaded bands represent the total pre-fit uncertainty on the prediction. The uncertainty does not include the normalization of the main backgrounds, which is unconstrained in the fit.
Data compared to the background prediction in each region of the negative $\lambda_{WZ}$ analysis, after the fit to data. The fitted signal strength is $\hat{\mu} = -0.027$, corresponding to $-8$ events. This contribution is not shown in the figure. The predicted signal yield with $\kappa_{W} = +1$, $\kappa_{Z} = +1$ in SR$^{-}$ is 2.93 events, which is also not shown in the figure. The shaded bands represent the total post-fit uncertainty on the prediction.
Data compared to the SM prediction in each region of the positive \lam{} analysis, before the fit to data. The shaded bands represent the total pre-fit uncertainty on the prediction. The uncertainty does not include the normalization of the main backgrounds, which is unconstrained in the fit.
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 is presented for the pair production of higgsinos $\tilde{\chi}$ in gauge-mediated supersymmetry models, where the lightest neutralinos $\tilde{\chi}_1^0$ decay into a light gravitino $\tilde{G}$ in association with either a Higgs $h$ or a $Z$ boson. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. It targets final states in which a Higgs boson decays into a photon pair, while the other Higgs or $Z$ boson decays into a $b\bar{b}$ pair, with missing transverse momentum associated with the two gravitinos. Search regions dependent on the amount of missing transverse momentum are defined by the requirements that the diphoton mass should be consistent with the mass of the Higgs boson, and the $b\bar{b}$ mass with the mass of the Higgs or $Z$ boson. The main backgrounds are estimated with data-driven methods using the sidebands of the diphoton mass distribution. No excesses beyond Standard Model expectations are observed and higgsinos with masses up to 320 GeV are excluded, assuming a branching fraction of 100% for $\tilde{\chi}_1^0\rightarrow h\tilde{G}$. This analysis excludes higgsinos with masses of 130 GeV for branching fractions to $h\tilde{G}$ as low as 36%, thus providing complementarity to previous ATLAS searches in final states with multiple leptons or multiple $b$-jets, targeting different decays of the electroweak bosons.
<b>- - - - - - - - Overview of HEPData Record - - - - - - - -</b> <b>Histograms:</b><ul> <li><a href=?table=Distribution1>Figure 3a: $m_{\gamma\gamma}$ Distribution in VR1</a> <li><a href=?table=Distribution2>Figure 3b: $E_{\mathrm{T}}^{\mathrm{miss}}$ Distribution in VR1</a> <li><a href=?table=Distribution3>Figure 3c: $m_{\gamma\gamma}$ Distribution in VR2</a> <li><a href=?table=Distribution4>Figure 3d: $E_{\mathrm{T}}^{\mathrm{miss}}$ Distribution in VR2</a> <li><a href=?table=Distribution5>Figure 4a: N-1 $m_{\gamma\gamma}$ Distribution for SR1h</a> <li><a href=?table=Distribution6>Figure 4b: N-1 $m_{\gamma\gamma}$ Distribution for SR1Z</a> <li><a href=?table=Distribution7>Figure 4c: N-1 $m_{\gamma\gamma}$ Distribution for SR2</a> <li><a href=?table=Distribution8>Auxiliary Figure 1: Signal and Validation Region Yields</a> </ul> <b>Tables:</b><ul> <li><a href=?table=YieldsTable1>Table 3: Signal Region Yields & Model-independent Limits</a> <li><a href=?table=Cutflow1>Auxiliary Table 1: Benchmark Signal Cutflows</a> </ul> <b>Cross section limits:</b><ul> <li><a href=?table=X-sectionU.L.1>Figure 5: 1D Cross-section Limits</a> <li><a href=?table=X-sectionU.L.2>Auxiliary Figure 3: 2D Cross-section Limits</a> </ul> <b>2D CL limits:</b><ul> <li><a href=?table=Exclusioncontour1>Figure 6: Expected Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> <li><a href=?table=Exclusioncontour2>Figure 6: $+1\sigma$ Variation for Expected Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> <li><a href=?table=Exclusioncontour3>Figure 6: $-1\sigma$ Variation for Expected Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> <li><a href=?table=Exclusioncontour4>Figure 6: Observed Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> <li><a href=?table=Exclusioncontour5>Figure 6: $+1\sigma$ Variation for Observed Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> <li><a href=?table=Exclusioncontour6>Figure 6: $-1\sigma$ Variation for Observed Limit on $\mathrm{BF}(\tilde{\chi}_1^0\rightarrow h\tilde{G})$</a> </ul> <b>2D Acceptance and Efficiency maps:</b><ul> <li><a href=?table=Acceptance1>Auxiliary Figure 4a: Acceptances SR1h</a> <li><a href=?table=Acceptance2>Auxiliary Figure 4b: Acceptances SR1Z</a> <li><a href=?table=Acceptance3>Auxiliary Figure 4c: Acceptances SR2</a> <li><a href=?table=Efficiency1>Auxiliary Figure 5a: Efficiencies SR1h</a> <li><a href=?table=Efficiency2>Auxiliary Figure 5b: Efficiencies SR1Z</a> <li><a href=?table=Efficiency3>Auxiliary Figure 5c: Efficiencies SR2</a> </ul>
Distribution of the diphoton invariant mass in validation region VR1. The solid histograms are stacked to show the SM expectations after the 2×2D background estimation technique is applied. Background and signal predictions are normalised to the luminosity. The background category "h (other)" includes events originating from VBF, Vh, ggF, thq, thW and bb̄h, all subdominant in this signature. Statistical and systematic uncertainties are indicated by the shaded area. The lower panel of each plot shows the ratio of the data to the SM prediction for the respective bin. The first and last bins include the underflows and overflows respectively.
Distribution of the missing transverse momentum in validation region VR1. The solid histograms are stacked to show the SM expectations after the 2×2D background estimation technique is applied. Background and signal predictions are normalised to the luminosity. The background category "h (other)" includes events originating from VBF, Vh, ggF, thq, thW and bb̄h, all subdominant in this signature. Statistical and systematic uncertainties are indicated by the shaded area. The lower panel of each plot shows the ratio of the data to the SM prediction for the respective bin. The first and last bins include the underflows and overflows respectively.
This Letter presents the first study of Higgs boson production in association with a vector boson (V = W or Z) in the fully hadronic $qqbb$ final state using data recorded by the ATLAS detector at the LHC in proton-proton collisions at $\sqrt{s}=13$ TeV and corresponding to an integrated luminosity of 137 fb$^{-1}$. The vector bosons and Higgs bosons are each reconstructed as large-radius jets and tagged using jet substructure techniques. Dedicated tagging algorithms exploiting $b$-tagging properties are used to identify jets consistent with Higgs bosons decaying into $b\bar{b}$. Dominant backgrounds from multijet production are determined directly from the data, and a likelihood fit to the jet mass distribution of Higgs boson candidates is used to extract the number of signal events. The VH production cross section is measured inclusively and differentially in several ranges of Higgs boson transverse momentum: 250-450, 450-650, and greater than 650 GeV. The inclusive signal yield relative to the standard model expectation is observed to be $\mu = 1.4 ^{+1.0}_{-0.9}$ and the corresponding cross section is $3.1 \pm 1.3\, (stat.)\: ^{+1.8}_{-1.4}\, (syst.$) pb.
Higgs candidate jet mass distributions in the signal region for $p_{T,J}^H$ in [250,450) GeV obtained after the inclusive fit with a single Z+jets normalization factor and a single signal strength.
Higgs candidate jet mass distributions in the signal region for $p_{T,J}^H$ in [450,650) GeV obtained after the inclusive fit with a single Z+jets normalization factor and a single signal strength.
Higgs candidate jet mass distributions in the signal region for $p_{T,J}^H \geq 650$ GeV obtained after the inclusive fit with a single Z+jets normalization factor and a single signal strength.
This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly massless gravitino. The search targets events where each Higgs boson decays into $b\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and This paper presents a search for pair production of higgsinos, the supersymmetric partners of the Higgs bosons, in scenarios with gauge-mediated supersymmetry breaking. Each higgsino is assumed to decay into a Higgs boson and a nearly massless gravitino. The search targets events where each Higgs boson decays into $b\bar{b}$, leading to a reconstructed final state with at least three energetic $b$-jets and missing transverse momentum. Two complementary analysis channels are used, with each channel specifically targeting either low or high values of the higgsino mass. The low-mass (high-mass) channel exploits 126 (139) fb$^{-1}$ of $\sqrt{s}=13$ TeV data collected by the ATLAS detector during Run 2 of the Large Hadron Collider. No significant excess above the Standard Model prediction is found. At 95% confidence level, masses between 130 GeV and 940 GeV are excluded for higgsinos decaying exclusively into Higgs bosons and gravitinos. Exclusion limits as a function of the higgsino decay branching ratio to a Higgs boson are also reported.
Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.
Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.
Post-fit SR yields of the high-mass channel. The upper panel shows the observed number of events, as well the post-fit background predictions in each region. The bottom panel shows the ratio of the observed data and the total background prediction. The shaded areas correspond to the total statistical and systematic uncertainties obtained after the fit and described in Section 6.
Searches for new resonances are performed using an unsupervised anomaly-detection technique. Events with at least one electron or muon are selected from 140 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV recorded by ATLAS at the Large Hadron Collider. The approach involves training an autoencoder on data, and subsequently defining anomalous regions based on the reconstruction loss of the decoder. Studies focus on nine invariant mass spectra that contain pairs of objects consisting of one light jet or $b$-jet and either one lepton ($e$, $\mu$), photon, or second light jet or $b$-jet in the anomalous regions. No significant deviations from the background hypotheses are observed.
Distributions of the anomaly score from the AE for data and five benchmark BSM models. Their legends, from top to bottom, are; (1) charged Higgs boson production in association with a top quark, $tbH^{+}$ with $H^{+} \rightarrow t\bar{b}$; (2) a Kaluza-Klein gauge boson, $W_{KK}$, with the SM $W$ boson and a radion $\phi$; (3) a $Z'$ boson decaying to a composite lepton $E$ and $\ell$, with $E \rightarrow Z\ell$ with a mass of 0.5 TeV; (4) the SSM $W$'$\rightarrow W Z' \rightarrow \ell\nu q\bar{q}$; (5) a simplified dark-matter model with an $Z$ axial-vector mediator $Z' \rightarrow q\bar{q}$, where one of the quarks radiates a $W$ boson decaying to $\ell\nu$. The BSM predictions represent the expected number of events from 140 $fb^{-1}$ of data for heavy particle ($H^{+}$ ,$W_{KK}$ , $Z'$ , $W'$ and $Z'$, respectively) masses around 2 TeV. The distributions for the BSM models are smoothed to remove fluctuations due to low MC event counts. The vertical lines indicate the start of the three anomaly regions (ARs). The labels of the three ARs indicate the visible cross section for hypothetical processes yielding the same number of events as observed in the 140 $fb^{-1}$ dataset. The AE is applied to preselected events without any requirements on invariant mass distributions.
Invariant mass distributions of jet+Y for $M_{jY}$ > 0.3 TeV in the 10 pb AR along with the fit of Eq. (1). The fits are represented by the lines, while the associated statistical uncertainties are indicated by the shaded bands. The lower panels show the bin-by-bin significances of deviations from the fit, calculated as $(d_{\textit{i}} - f_{i})/\delta_{\textit{i}}$, where $d_{i}$ is the data yield, $f_{\textit{i}}$ is the fit value, and $\delta_{i}$ is the data uncertainty in the $\textit{i}$-th bin.
Values of $\Delta Z$ for the discovery sensitivity, as defined in the text, as a function of the invariant mass $\textit{m}$. The j+j invariant mass distribution is calculated in the 10 pb AR. Positive percentages indicate improvements in sensitivity. Horizontal dashed lines are drawn at 100% and 200% to guide the eye. The five benchmark BSM models are (1) charged Higgs boson production in association with a top quark, $tbH^{+}$ with $H^{+} \rightarrow t\bar{b}$; (2) a Kaluza-Klein gauge boson, $W_{KK}$, with the SM $W$ boson and a radion $\phi$; (3) a $Z'$ boson decaying to a composite lepton $E$ and $\ell$, with $E \rightarrow Z\ell$; (4) the sequential standard model $W' \rightarrow W Z' \rightarrow \ell\nu q\bar{q}$; (5) a simplified dark-matter model with an axial-vector mediator $Z' \rightarrow q\bar{q}$, where one of the quarks radiates a $W$ boson decaying to $\ell\nu$. The multiple markers shown for the composite-lepton model at the same invariant mass values correspond to different composite lepton ($E$) masses between 0.25 and 3.5 TeV. The center positions of the markers are set to the masses of the corresponding heavy particles.
Parton energy loss in the quark-gluon plasma (QGP) is studied with a measurement of photon-tagged jet production in 1.7 nb$^{-1}$ of Pb+Pb data and 260 pb$^{-1}$ of $pp$ data, both at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV, with the ATLAS detector. The process $pp \to \gamma$+jet+$X$ and its analogue in Pb+Pb collisions is measured in events containing an isolated photon with transverse momentum ($p_\mathrm{T}$) above $50$ GeV and reported as a function of jet $p_\mathrm{T}$. This selection results in a sample of jets with a steeply falling $p_\mathrm{T}$ distribution that are mostly initiated by the showering of quarks. The $pp$ and Pb+Pb measurements are used to report the nuclear modification factor, $R_\mathrm{AA}$, and the fractional energy loss, $S_\mathrm{loss}$, for photon-tagged jets. In addition, the results are compared with the analogous ones for inclusive jets, which have a significantly smaller quark-initiated fraction. The $R_\mathrm{AA}$ and $S_\mathrm{loss}$ values are found to be significantly different between those for photon-tagged jets and inclusive jets, demonstrating that energy loss in the QGP is sensitive to the colour-charge of the initiating parton. The results are also compared with a variety of theoretical models of colour-charge-dependent energy loss.
The differential cross-section of photon-tagged jets as a function of jet $p_{\mathrm{T}}$ in pp collisions.
The yields of photon-tagged jets as a function of jet $p_{\mathrm{T}}$ in Pb+Pb collisions for different centrality intervals.
The nuclear modification factor of photon-tagged jets as a function of jet $p_{\mathrm{T}}$ for different centrality intervals.
Measurements of single-, double-, and triple-differential cross-sections are presented for boosted top-quark pair-production in 13 $\text{TeV}$ proton-proton collisions recorded by the ATLAS detector at the LHC. The top quarks are observed through their hadronic decay and reconstructed as large-radius jets with the leading jet having transverse momentum ($p_{\text{T}}$) greater than 500 GeV. The observed data are unfolded to remove detector effects. The particle-level cross-section, multiplied by the $t\bar{t} \rightarrow W W b \bar{b}$ branching fraction and measured in a fiducial phase space defined by requiring the leading and second-leading jets to have $p_{\text{T}} > 500$ GeV and $p_{\text{T}} > 350$ GeV, respectively, is $331 \pm 3 \text{(stat.)} \pm 39 \text{(syst.)}$ fb. This is approximately 20$\%$ lower than the prediction of $398^{+48}_{-49}$ fb by Powheg+Pythia 8 with next-to-leading-order (NLO) accuracy but consistent within the theoretical uncertainties. Results are also presented at the parton level, where the effects of top-quark decay, parton showering, and hadronization are removed such that they can be compared with fixed-order next-to-next-to-leading-order (NNLO) calculations. The parton-level cross-section, measured in a fiducial phase space similar to that at particle level, is $1.94 \pm 0.02 \text{(stat.)} \pm 0.25 \text{(syst.)}$ pb. This agrees with the NNLO prediction of $1.96^{+0.02}_{-0.17}$ pb. Reasonable agreement with the differential cross-sections is found for most NLO models, while the NNLO calculations are generally in better agreement with the data. The differential cross-sections are interpreted using a Standard Model effective field-theory formalism and limits are set on Wilson coefficients of several four-fermion operators.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definitions:</b><br/> <i>Particle level:</i> <ul> <li> NLEP = 0, E or MU, PT > 25 GeV, ABS ETA < 2.5 <li> NJETS >= 2, R = 1.0, 350 GeV < PT < 3000 GeV, ABS ETA < 2, M > 50 GeV <li> NJETS >= 1, R = 1.0, 500 GeV < PT < 3000 GeV, ABS ETA < 2, M > 50 GeV <li> T1, MIN ( ABS ( M - 172.5 GeV ) ), candidate JETS with PT > 500 GeV <li> T2, MIN ( ABS ( M - 172.5 GeV ) ), remaining candidate JETS with PT > 350 GeV <li> T1 and T2, 122.5 GeV < M < 222.5 GeV, ghost-matched B-HAD with PT > 5 GeV </ul><br/> <i>Parton level:</i> <ul> <li> PT_T1 > 500 GeV, PT_T2 > 350 GeV </ul><br/> <b>Particle level:</b><br/> <u>1D:</u><br/> Spectra: <ul><br/> <li>SIG (<a href="115142?table=Table 1">Table 1</a>) <li>DSIG/DPT_TOP (<a href="115142?table=Table 2">Table 2</a>) <li>DSIG/DABS_Y_TOP (<a href="115142?table=Table 3">Table 3</a>) <li>DSIG/DPT_T1 (<a href="115142?table=Table 4">Table 4</a>) <li>DSIG/DABS_Y_T1 (<a href="115142?table=Table 5">Table 5</a>) <li>DSIG/DPT_T2 (<a href="115142?table=Table 6">Table 6</a>) <li>DSIG/DABS_Y_T2 (<a href="115142?table=Table 7">Table 7</a>) <li>DSIG/DM_TTBAR (<a href="115142?table=Table 8">Table 8</a>) <li>DSIG/DPT_TTBAR (<a href="115142?table=Table 9">Table 9</a>) <li>DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 10">Table 10</a>) <li>DSIG/DCHI_TTBAR (<a href="115142?table=Table 11">Table 11</a>) <li>DSIG/DABS_Y_BOOST (<a href="115142?table=Table 12">Table 12</a>) <li>DSIG/DABS_POUT (<a href="115142?table=Table 13">Table 13</a>) <li>DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 14">Table 14</a>) <li>DSIG/DHT_TTBAR (<a href="115142?table=Table 15">Table 15</a>) <li>DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 16">Table 16</a>) <li>1/SIG*DSIG/DPT_TOP (<a href="115142?table=Table 74">Table 74</a>) <li>1/SIG*DSIG/DABS_Y_TOP (<a href="115142?table=Table 75">Table 75</a>) <li>1/SIG*DSIG/DPT_T1 (<a href="115142?table=Table 76">Table 76</a>) <li>1/SIG*DSIG/DABS_Y_T1 (<a href="115142?table=Table 77">Table 77</a>) <li>1/SIG*DSIG/DPT_T2 (<a href="115142?table=Table 78">Table 78</a>) <li>1/SIG*DSIG/DABS_Y_T2 (<a href="115142?table=Table 79">Table 79</a>) <li>1/SIG*DSIG/DM_TTBAR (<a href="115142?table=Table 80">Table 80</a>) <li>1/SIG*DSIG/DPT_TTBAR (<a href="115142?table=Table 81">Table 81</a>) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 82">Table 82</a>) <li>1/SIG*DSIG/DCHI_TTBAR (<a href="115142?table=Table 83">Table 83</a>) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="115142?table=Table 84">Table 84</a>) <li>1/SIG*DSIG/DABS_POUT (<a href="115142?table=Table 85">Table 85</a>) <li>1/SIG*DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 86">Table 86</a>) <li>1/SIG*DSIG/DHT_TTBAR (<a href="115142?table=Table 87">Table 87</a>) <li>1/SIG*DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 88">Table 88</a>) </ul><br/> Covariances: <ul><br/> <li>DSIG/DPT_TOP (<a href="115142?table=Table 291">Table 291</a>) <li>DSIG/DABS_Y_TOP (<a href="115142?table=Table 292">Table 292</a>) <li>DSIG/DPT_T1 (<a href="115142?table=Table 293">Table 293</a>) <li>DSIG/DABS_Y_T1 (<a href="115142?table=Table 294">Table 294</a>) <li>DSIG/DPT_T2 (<a href="115142?table=Table 295">Table 295</a>) <li>DSIG/DABS_Y_T2 (<a href="115142?table=Table 296">Table 296</a>) <li>DSIG/DM_TTBAR (<a href="115142?table=Table 297">Table 297</a>) <li>DSIG/DPT_TTBAR (<a href="115142?table=Table 298">Table 298</a>) <li>DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 299">Table 299</a>) <li>DSIG/DCHI_TTBAR (<a href="115142?table=Table 300">Table 300</a>) <li>DSIG/DABS_Y_BOOST (<a href="115142?table=Table 301">Table 301</a>) <li>DSIG/DABS_POUT (<a href="115142?table=Table 302">Table 302</a>) <li>DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 303">Table 303</a>) <li>DSIG/DHT_TTBAR (<a href="115142?table=Table 304">Table 304</a>) <li>DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 305">Table 305</a>) <li>1/SIG*DSIG/DPT_TOP (<a href="115142?table=Table 471">Table 471</a>) <li>1/SIG*DSIG/DABS_Y_TOP (<a href="115142?table=Table 472">Table 472</a>) <li>1/SIG*DSIG/DPT_T1 (<a href="115142?table=Table 473">Table 473</a>) <li>1/SIG*DSIG/DABS_Y_T1 (<a href="115142?table=Table 474">Table 474</a>) <li>1/SIG*DSIG/DPT_T2 (<a href="115142?table=Table 475">Table 475</a>) <li>1/SIG*DSIG/DABS_Y_T2 (<a href="115142?table=Table 476">Table 476</a>) <li>1/SIG*DSIG/DM_TTBAR (<a href="115142?table=Table 477">Table 477</a>) <li>1/SIG*DSIG/DPT_TTBAR (<a href="115142?table=Table 478">Table 478</a>) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 479">Table 479</a>) <li>1/SIG*DSIG/DCHI_TTBAR (<a href="115142?table=Table 480">Table 480</a>) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="115142?table=Table 481">Table 481</a>) <li>1/SIG*DSIG/DABS_POUT (<a href="115142?table=Table 482">Table 482</a>) <li>1/SIG*DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 483">Table 483</a>) <li>1/SIG*DSIG/DHT_TTBAR (<a href="115142?table=Table 484">Table 484</a>) <li>1/SIG*DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 485">Table 485</a>) </ul><br/> <u>2D:</u><br/> Spectra: <ul><br/> <li>D2SIG/DPT_T2/DPT_T1 (0.50 TeV < PT_T1 < 0.55 TeV) (<a href="115142?table=Table 17">Table 17</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.55 TeV < PT_T1 < 0.60 TeV) (<a href="115142?table=Table 18">Table 18</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.60 TeV < PT_T1 < 0.75 TeV) (<a href="115142?table=Table 19">Table 19</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.75 TeV < PT_T1 < 2.00 TeV) (<a href="115142?table=Table 20">Table 20</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 21">Table 21</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 22">Table 22</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 23">Table 23</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 24">Table 24</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 25">Table 25</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 26">Table 26</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 27">Table 27</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 28">Table 28</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.0 < ABS_Y_T2 < 0.2) (<a href="115142?table=Table 29">Table 29</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.2 < ABS_Y_T2 < 0.5) (<a href="115142?table=Table 30">Table 30</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.5 < ABS_Y_T2 < 1.0) (<a href="115142?table=Table 31">Table 31</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (1.0 < ABS_Y_T2 < 2.0) (<a href="115142?table=Table 32">Table 32</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 33">Table 33</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 34">Table 34</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 35">Table 35</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 36">Table 36</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 37">Table 37</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 38">Table 38</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 39">Table 39</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 40">Table 40</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 41">Table 41</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 42">Table 42</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 43">Table 43</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 44">Table 44</a>) <li>D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 45">Table 45</a>) <li>D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 46">Table 46</a>) <li>D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 47">Table 47</a>) <li>D2SIG/DABS_Y_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 48">Table 48</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 49">Table 49</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 50">Table 50</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 51">Table 51</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 52">Table 52</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 53">Table 53</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 54">Table 54</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 55">Table 55</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 56">Table 56</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.00 TeV < PT_TTBAR < 0.10 TeV) (<a href="115142?table=Table 57">Table 57</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.10 TeV < PT_TTBAR < 0.20 TeV) (<a href="115142?table=Table 58">Table 58</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.20 TeV < PT_TTBAR < 0.35 TeV) (<a href="115142?table=Table 59">Table 59</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.35 TeV < PT_TTBAR < 1.00 TeV) (<a href="115142?table=Table 60">Table 60</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 61">Table 61</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 62">Table 62</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 63">Table 63</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 64">Table 64</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.50 TeV < PT_T1 < 0.55 TeV) (<a href="115142?table=Table 89">Table 89</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.55 TeV < PT_T1 < 0.60 TeV) (<a href="115142?table=Table 90">Table 90</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.60 TeV < PT_T1 < 0.75 TeV) (<a href="115142?table=Table 91">Table 91</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.75 TeV < PT_T1 < 2.00 TeV) (<a href="115142?table=Table 92">Table 92</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 93">Table 93</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 94">Table 94</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 95">Table 95</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 96">Table 96</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 97">Table 97</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 98">Table 98</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 99">Table 99</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 100">Table 100</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.0 < ABS_Y_T2 < 0.2) (<a href="115142?table=Table 101">Table 101</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.2 < ABS_Y_T2 < 0.5) (<a href="115142?table=Table 102">Table 102</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.5 < ABS_Y_T2 < 1.0) (<a href="115142?table=Table 103">Table 103</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (1.0 < ABS_Y_T2 < 2.0) (<a href="115142?table=Table 104">Table 104</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 105">Table 105</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 106">Table 106</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 107">Table 107</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 108">Table 108</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 109">Table 109</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 110">Table 110</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 111">Table 111</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 112">Table 112</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 113">Table 113</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 114">Table 114</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 115">Table 115</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 116">Table 116</a>) <li>1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 117">Table 117</a>) <li>1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 118">Table 118</a>) <li>1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 119">Table 119</a>) <li>1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 120">Table 120</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 121">Table 121</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 122">Table 122</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 123">Table 123</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 124">Table 124</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 125">Table 125</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 126">Table 126</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 127">Table 127</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 128">Table 128</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.00 TeV < PT_TTBAR < 0.10 TeV) (<a href="115142?table=Table 129">Table 129</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.10 TeV < PT_TTBAR < 0.20 TeV) (<a href="115142?table=Table 130">Table 130</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.20 TeV < PT_TTBAR < 0.35 TeV) (<a href="115142?table=Table 131">Table 131</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.35 TeV < PT_TTBAR < 1.00 TeV) (<a href="115142?table=Table 132">Table 132</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 133">Table 133</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 134">Table 134</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 135">Table 135</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 136">Table 136</a>) </ul><br/> Covariances: <ul><br/> <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 306">Table 306</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 307">Table 307</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 308">Table 308</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 309">Table 309</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 310">Table 310</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 311">Table 311</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 312">Table 312</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 313">Table 313</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 314">Table 314</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 315">Table 315</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 316">Table 316</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 317">Table 317</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 318">Table 318</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 319">Table 319</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 320">Table 320</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 321">Table 321</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 322">Table 322</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 323">Table 323</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 324">Table 324</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 325">Table 325</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 326">Table 326</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 327">Table 327</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 328">Table 328</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 329">Table 329</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 330">Table 330</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 331">Table 331</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 332">Table 332</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 333">Table 333</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 334">Table 334</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 335">Table 335</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 1st bins of ABS_Y_T2 (<a href="115142?table=Table 336">Table 336</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 337">Table 337</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 338">Table 338</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 339">Table 339</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 340">Table 340</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 341">Table 341</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 342">Table 342</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 343">Table 343</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 344">Table 344</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 4th and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 345">Table 345</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 346">Table 346</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 347">Table 347</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 348">Table 348</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 349">Table 349</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 350">Table 350</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 351">Table 351</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 352">Table 352</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 353">Table 353</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 354">Table 354</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 355">Table 355</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 356">Table 356</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 357">Table 357</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 358">Table 358</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 359">Table 359</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 360">Table 360</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 361">Table 361</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 362">Table 362</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 363">Table 363</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 364">Table 364</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 365">Table 365</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 366">Table 366</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 367">Table 367</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 368">Table 368</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 369">Table 369</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 370">Table 370</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 371">Table 371</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 372">Table 372</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 373">Table 373</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 374">Table 374</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 375">Table 375</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 376">Table 376</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 377">Table 377</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 378">Table 378</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 379">Table 379</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 380">Table 380</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 381">Table 381</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 382">Table 382</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 383">Table 383</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 384">Table 384</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 385">Table 385</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 386">Table 386</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 387">Table 387</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 388">Table 388</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 389">Table 389</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 390">Table 390</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 391">Table 391</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 392">Table 392</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 393">Table 393</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 394">Table 394</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 395">Table 395</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 396">Table 396</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 397">Table 397</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 398">Table 398</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 399">Table 399</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 400">Table 400</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 401">Table 401</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 402">Table 402</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 403">Table 403</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 404">Table 404</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 405">Table 405</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 1st bins of PT_TTBAR (<a href="115142?table=Table 406">Table 406</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 2nd bins of PT_TTBAR (<a href="115142?table=Table 407">Table 407</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 3rd bins of PT_TTBAR (<a href="115142?table=Table 408">Table 408</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 4th bins of PT_TTBAR (<a href="115142?table=Table 409">Table 409</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 2nd bins of PT_TTBAR (<a href="115142?table=Table 410">Table 410</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 411">Table 411</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 4th bins of PT_TTBAR (<a href="115142?table=Table 412">Table 412</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 413">Table 413</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 4th bins of PT_TTBAR (<a href="115142?table=Table 414">Table 414</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="115142?table=Table 415">Table 415</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 416">Table 416</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 417">Table 417</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 418">Table 418</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 419">Table 419</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 420">Table 420</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 421">Table 421</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 422">Table 422</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 423">Table 423</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 424">Table 424</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 425">Table 425</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 486">Table 486</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 487">Table 487</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 488">Table 488</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 489">Table 489</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 490">Table 490</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 491">Table 491</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 492">Table 492</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 493">Table 493</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 494">Table 494</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 495">Table 495</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 496">Table 496</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 497">Table 497</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 498">Table 498</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 499">Table 499</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 500">Table 500</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 501">Table 501</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 502">Table 502</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 503">Table 503</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 504">Table 504</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 505">Table 505</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 506">Table 506</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 507">Table 507</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 508">Table 508</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 509">Table 509</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 510">Table 510</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 511">Table 511</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 512">Table 512</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 513">Table 513</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 514">Table 514</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 515">Table 515</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 1st bins of ABS_Y_T2 (<a href="115142?table=Table 516">Table 516</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 517">Table 517</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 518">Table 518</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 519">Table 519</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 520">Table 520</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 521">Table 521</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 522">Table 522</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 523">Table 523</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 524">Table 524</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 4th and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 525">Table 525</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 526">Table 526</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 527">Table 527</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 528">Table 528</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 529">Table 529</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 530">Table 530</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 531">Table 531</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 532">Table 532</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 533">Table 533</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 534">Table 534</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 535">Table 535</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 536">Table 536</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 537">Table 537</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 538">Table 538</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 539">Table 539</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 540">Table 540</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 541">Table 541</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 542">Table 542</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 543">Table 543</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 544">Table 544</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 545">Table 545</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 546">Table 546</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 547">Table 547</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 548">Table 548</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 549">Table 549</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 550">Table 550</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 551">Table 551</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 552">Table 552</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 553">Table 553</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 554">Table 554</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 555">Table 555</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 556">Table 556</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 557">Table 557</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 558">Table 558</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 559">Table 559</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 560">Table 560</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 561">Table 561</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 562">Table 562</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 563">Table 563</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 564">Table 564</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 565">Table 565</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 566">Table 566</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 567">Table 567</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 568">Table 568</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 569">Table 569</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 570">Table 570</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 571">Table 571</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 572">Table 572</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 573">Table 573</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 574">Table 574</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 575">Table 575</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 576">Table 576</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 577">Table 577</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 578">Table 578</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 579">Table 579</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 580">Table 580</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 581">Table 581</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 582">Table 582</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 583">Table 583</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 584">Table 584</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 585">Table 585</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 1st bins of PT_TTBAR (<a href="115142?table=Table 586">Table 586</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 2nd bins of PT_TTBAR (<a href="115142?table=Table 587">Table 587</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 3rd bins of PT_TTBAR (<a href="115142?table=Table 588">Table 588</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 4th bins of PT_TTBAR (<a href="115142?table=Table 589">Table 589</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 2nd bins of PT_TTBAR (<a href="115142?table=Table 590">Table 590</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 591">Table 591</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 4th bins of PT_TTBAR (<a href="115142?table=Table 592">Table 592</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 593">Table 593</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 4th bins of PT_TTBAR (<a href="115142?table=Table 594">Table 594</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="115142?table=Table 595">Table 595</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 596">Table 596</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 597">Table 597</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 598">Table 598</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 599">Table 599</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 600">Table 600</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 601">Table 601</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 602">Table 602</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 603">Table 603</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 604">Table 604</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 605">Table 605</a>) </ul><br/> <u>3D:</u><br/> Spectra: <ul><br/> <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 65">Table 65</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 66">Table 66</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 67">Table 67</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 68">Table 68</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 69">Table 69</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 70">Table 70</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 71">Table 71</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 72">Table 72</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 73">Table 73</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 137">Table 137</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 138">Table 138</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 139">Table 139</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 140">Table 140</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 141">Table 141</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 142">Table 142</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 143">Table 143</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 144">Table 144</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 145">Table 145</a>) </ul><br/> Covariances: <ul><br/> <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 426">Table 426</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 427">Table 427</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 428">Table 428</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 429">Table 429</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 430">Table 430</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 431">Table 431</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 432">Table 432</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 433">Table 433</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 434">Table 434</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 435">Table 435</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 436">Table 436</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 437">Table 437</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 438">Table 438</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 439">Table 439</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 440">Table 440</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 441">Table 441</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 442">Table 442</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 443">Table 443</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 444">Table 444</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 445">Table 445</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 446">Table 446</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 447">Table 447</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 448">Table 448</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 449">Table 449</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 450">Table 450</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 451">Table 451</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 452">Table 452</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 453">Table 453</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 454">Table 454</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 455">Table 455</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 456">Table 456</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 457">Table 457</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 458">Table 458</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 459">Table 459</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 460">Table 460</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 461">Table 461</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 462">Table 462</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 463">Table 463</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 464">Table 464</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 465">Table 465</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 466">Table 466</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 467">Table 467</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 468">Table 468</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 469">Table 469</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 470">Table 470</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 606">Table 606</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 607">Table 607</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 608">Table 608</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 609">Table 609</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 610">Table 610</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 611">Table 611</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 612">Table 612</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 613">Table 613</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 614">Table 614</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 615">Table 615</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 616">Table 616</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 617">Table 617</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 618">Table 618</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 619">Table 619</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 620">Table 620</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 621">Table 621</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 622">Table 622</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 623">Table 623</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 624">Table 624</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 625">Table 625</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 626">Table 626</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 627">Table 627</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 628">Table 628</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 629">Table 629</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 630">Table 630</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 631">Table 631</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 632">Table 632</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 633">Table 633</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 634">Table 634</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 635">Table 635</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 636">Table 636</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 637">Table 637</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 638">Table 638</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 639">Table 639</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 640">Table 640</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 641">Table 641</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 642">Table 642</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 643">Table 643</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 644">Table 644</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 645">Table 645</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 646">Table 646</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 647">Table 647</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 648">Table 648</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 649">Table 649</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 650">Table 650</a>) </ul><br/> <b>Parton level:</b><br/> <u>1D:</u><br/> Spectra: <ul><br/> <li>SIG (<a href="115142?table=Table 146">Table 146</a>) <li>DSIG/DPT_TOP (<a href="115142?table=Table 147">Table 147</a>) <li>DSIG/DABS_Y_TOP (<a href="115142?table=Table 148">Table 148</a>) <li>DSIG/DPT_T1 (<a href="115142?table=Table 149">Table 149</a>) <li>DSIG/DABS_Y_T1 (<a href="115142?table=Table 150">Table 150</a>) <li>DSIG/DPT_T2 (<a href="115142?table=Table 151">Table 151</a>) <li>DSIG/DABS_Y_T2 (<a href="115142?table=Table 152">Table 152</a>) <li>DSIG/DM_TTBAR (<a href="115142?table=Table 153">Table 153</a>) <li>DSIG/DPT_TTBAR (<a href="115142?table=Table 154">Table 154</a>) <li>DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 155">Table 155</a>) <li>DSIG/DCHI_TTBAR (<a href="115142?table=Table 156">Table 156</a>) <li>DSIG/DABS_Y_BOOST (<a href="115142?table=Table 157">Table 157</a>) <li>DSIG/DABS_POUT (<a href="115142?table=Table 158">Table 158</a>) <li>DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 159">Table 159</a>) <li>DSIG/DHT_TTBAR (<a href="115142?table=Table 160">Table 160</a>) <li>DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 161">Table 161</a>) <li>1/SIG*DSIG/DPT_TOP (<a href="115142?table=Table 219">Table 219</a>) <li>1/SIG*DSIG/DABS_Y_TOP (<a href="115142?table=Table 220">Table 220</a>) <li>1/SIG*DSIG/DPT_T1 (<a href="115142?table=Table 221">Table 221</a>) <li>1/SIG*DSIG/DABS_Y_T1 (<a href="115142?table=Table 222">Table 222</a>) <li>1/SIG*DSIG/DPT_T2 (<a href="115142?table=Table 223">Table 223</a>) <li>1/SIG*DSIG/DABS_Y_T2 (<a href="115142?table=Table 224">Table 224</a>) <li>1/SIG*DSIG/DM_TTBAR (<a href="115142?table=Table 225">Table 225</a>) <li>1/SIG*DSIG/DPT_TTBAR (<a href="115142?table=Table 226">Table 226</a>) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 227">Table 227</a>) <li>1/SIG*DSIG/DCHI_TTBAR (<a href="115142?table=Table 228">Table 228</a>) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="115142?table=Table 229">Table 229</a>) <li>1/SIG*DSIG/DABS_POUT (<a href="115142?table=Table 230">Table 230</a>) <li>1/SIG*DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 231">Table 231</a>) <li>1/SIG*DSIG/DHT_TTBAR (<a href="115142?table=Table 232">Table 232</a>) <li>1/SIG*DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 233">Table 233</a>) </ul><br/> Covariances: <ul><br/> <li>DSIG/DPT_TOP (<a href="115142?table=Table 651">Table 651</a>) <li>DSIG/DABS_Y_TOP (<a href="115142?table=Table 652">Table 652</a>) <li>DSIG/DPT_T1 (<a href="115142?table=Table 653">Table 653</a>) <li>DSIG/DABS_Y_T1 (<a href="115142?table=Table 654">Table 654</a>) <li>DSIG/DPT_T2 (<a href="115142?table=Table 655">Table 655</a>) <li>DSIG/DABS_Y_T2 (<a href="115142?table=Table 656">Table 656</a>) <li>DSIG/DM_TTBAR (<a href="115142?table=Table 657">Table 657</a>) <li>DSIG/DPT_TTBAR (<a href="115142?table=Table 658">Table 658</a>) <li>DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 659">Table 659</a>) <li>DSIG/DCHI_TTBAR (<a href="115142?table=Table 660">Table 660</a>) <li>DSIG/DABS_Y_BOOST (<a href="115142?table=Table 661">Table 661</a>) <li>DSIG/DABS_POUT (<a href="115142?table=Table 662">Table 662</a>) <li>DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 663">Table 663</a>) <li>DSIG/DHT_TTBAR (<a href="115142?table=Table 664">Table 664</a>) <li>DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 665">Table 665</a>) <li>1/SIG*DSIG/DPT_TOP (<a href="115142?table=Table 831">Table 831</a>) <li>1/SIG*DSIG/DABS_Y_TOP (<a href="115142?table=Table 832">Table 832</a>) <li>1/SIG*DSIG/DPT_T1 (<a href="115142?table=Table 833">Table 833</a>) <li>1/SIG*DSIG/DABS_Y_T1 (<a href="115142?table=Table 834">Table 834</a>) <li>1/SIG*DSIG/DPT_T2 (<a href="115142?table=Table 835">Table 835</a>) <li>1/SIG*DSIG/DABS_Y_T2 (<a href="115142?table=Table 836">Table 836</a>) <li>1/SIG*DSIG/DM_TTBAR (<a href="115142?table=Table 837">Table 837</a>) <li>1/SIG*DSIG/DPT_TTBAR (<a href="115142?table=Table 838">Table 838</a>) <li>1/SIG*DSIG/DABS_Y_TTBAR (<a href="115142?table=Table 839">Table 839</a>) <li>1/SIG*DSIG/DCHI_TTBAR (<a href="115142?table=Table 840">Table 840</a>) <li>1/SIG*DSIG/DABS_Y_BOOST (<a href="115142?table=Table 841">Table 841</a>) <li>1/SIG*DSIG/DABS_POUT (<a href="115142?table=Table 842">Table 842</a>) <li>1/SIG*DSIG/DABS_DPHI_TTBAR (<a href="115142?table=Table 843">Table 843</a>) <li>1/SIG*DSIG/DHT_TTBAR (<a href="115142?table=Table 844">Table 844</a>) <li>1/SIG*DSIG/DABS_COS_THETA_STAR (<a href="115142?table=Table 845">Table 845</a>) </ul><br/> <u>2D:</u><br/> Spectra: <ul><br/> <li>D2SIG/DPT_T2/DPT_T1 (0.50 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 162">Table 162</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.55 TeV < PT_T1 < 0.60 TeV) (<a href="115142?table=Table 163">Table 163</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.60 TeV < PT_T1 < 0.75 TeV) (<a href="115142?table=Table 164">Table 164</a>) <li>D2SIG/DPT_T2/DPT_T1 (0.75 TeV < PT_T1 < 2.00 TeV) (<a href="115142?table=Table 165">Table 165</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 166">Table 166</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 167">Table 167</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 168">Table 168</a>) <li>D2SIG/DABS_Y_T2/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 169">Table 169</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 170">Table 170</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 171">Table 171</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 172">Table 172</a>) <li>D2SIG/DPT_T1/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 173">Table 173</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.0 < ABS_Y_T2 < 0.2) (<a href="115142?table=Table 174">Table 174</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.2 < ABS_Y_T2 < 0.5) (<a href="115142?table=Table 175">Table 175</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (0.5 < ABS_Y_T2 < 1.0) (<a href="115142?table=Table 176">Table 176</a>) <li>D2SIG/DPT_T2/DABS_Y_T2 (1.0 < ABS_Y_T2 < 2.0) (<a href="115142?table=Table 177">Table 177</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 178">Table 178</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 179">Table 179</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 180">Table 180</a>) <li>D2SIG/DPT_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 181">Table 181</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 182">Table 182</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 183">Table 183</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 184">Table 184</a>) <li>D2SIG/DM_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 185">Table 185</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 186">Table 186</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 187">Table 187</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 188">Table 188</a>) <li>D2SIG/DPT_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 189">Table 189</a>) <li>D2SIG/DY_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 190">Table 190</a>) <li>D2SIG/DY_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 191">Table 191</a>) <li>D2SIG/DY_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 192">Table 192</a>) <li>D2SIG/DY_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 193">Table 193</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 194">Table 194</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 195">Table 195</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 196">Table 196</a>) <li>D2SIG/DM_TTBAR/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 197">Table 197</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 198">Table 198</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 199">Table 199</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 200">Table 200</a>) <li>D2SIG/DM_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 201">Table 201</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.00 TeV < PT_TTBAR < 0.10 TeV) (<a href="115142?table=Table 202">Table 202</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.10 TeV < PT_TTBAR < 0.20 TeV) (<a href="115142?table=Table 203">Table 203</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.20 TeV < PT_TTBAR < 0.35 TeV) (<a href="115142?table=Table 204">Table 204</a>) <li>D2SIG/DM_TTBAR/PT_TTBAR (0.35 TeV < PT_TTBAR < 1.00 TeV) (<a href="115142?table=Table 205">Table 205</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 206">Table 206</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 207">Table 207</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 208">Table 208</a>) <li>D2SIG/PT_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 209">Table 209</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.50 TeV < PT_T1 < 0.55 TeV) (<a href="115142?table=Table 234">Table 234</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.55 TeV < PT_T1 < 0.60 TeV) (<a href="115142?table=Table 235">Table 235</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.60 TeV < PT_T1 < 0.75 TeV) (<a href="115142?table=Table 236">Table 236</a>) <li>1/SIG*D2SIG/DPT_T2/DPT_T1 (0.75 TeV < PT_T1 < 2.00 TeV) (<a href="115142?table=Table 237">Table 237</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 238">Table 238</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 239">Table 239</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 240">Table 240</a>) <li>1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 241">Table 241</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 242">Table 242</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 243">Table 243</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 244">Table 244</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 245">Table 245</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.0 < ABS_Y_T2 < 0.2) (<a href="115142?table=Table 246">Table 246</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.2 < ABS_Y_T2 < 0.5) (<a href="115142?table=Table 247">Table 247</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (0.5 < ABS_Y_T2 < 1.0) (<a href="115142?table=Table 248">Table 248</a>) <li>1/SIG*D2SIG/DPT_T2/DABS_Y_T2 (1.0 < ABS_Y_T2 < 2.0) (<a href="115142?table=Table 249">Table 249</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 250">Table 250</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 251">Table 251</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 252">Table 252</a>) <li>1/SIG*D2SIG/DPT_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 253">Table 253</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.500 TeV < PT_T1 < 0.550 TeV) (<a href="115142?table=Table 254">Table 254</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.550 TeV < PT_T1 < 0.625 TeV) (<a href="115142?table=Table 255">Table 255</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.625 TeV < PT_T1 < 0.750 TeV) (<a href="115142?table=Table 256">Table 256</a>) <li>1/SIG*D2SIG/DM_TTBAR/DPT_T1 (0.750 TeV < PT_T1 < 2.000 TeV) (<a href="115142?table=Table 257">Table 257</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 258">Table 258</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 259">Table 259</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 260">Table 260</a>) <li>1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 261">Table 261</a>) <li>1/SIG*D2SIG/DY_T1/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 262">Table 262</a>) <li>1/SIG*D2SIG/DY_T1/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 263">Table 263</a>) <li>1/SIG*D2SIG/DY_T1/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 264">Table 264</a>) <li>1/SIG*D2SIG/DY_T1/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 265">Table 265</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.0 < ABS_Y_T1 < 0.2) (<a href="115142?table=Table 266">Table 266</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.2 < ABS_Y_T1 < 0.5) (<a href="115142?table=Table 267">Table 267</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (0.5 < ABS_Y_T1 < 1.0) (<a href="115142?table=Table 268">Table 268</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 (1.0 < ABS_Y_T1 < 2.0) (<a href="115142?table=Table 269">Table 269</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 270">Table 270</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 271">Table 271</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 272">Table 272</a>) <li>1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 273">Table 273</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.00 TeV < PT_TTBAR < 0.10 TeV) (<a href="115142?table=Table 274">Table 274</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.10 TeV < PT_TTBAR < 0.20 TeV) (<a href="115142?table=Table 275">Table 275</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.20 TeV < PT_TTBAR < 0.35 TeV) (<a href="115142?table=Table 276">Table 276</a>) <li>1/SIG*D2SIG/DM_TTBAR/PT_TTBAR (0.35 TeV < PT_TTBAR < 1.00 TeV) (<a href="115142?table=Table 277">Table 277</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.0 < ABS_Y_TTBAR < 0.2) (<a href="115142?table=Table 278">Table 278</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.2 < ABS_Y_TTBAR < 0.5) (<a href="115142?table=Table 279">Table 279</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (0.5 < ABS_Y_TTBAR < 1.0) (<a href="115142?table=Table 280">Table 280</a>) <li>1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR (1.0 < ABS_Y_TTBAR < 2.0) (<a href="115142?table=Table 281">Table 281</a>) </ul><br/> Covariances: <ul><br/> <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 666">Table 666</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 667">Table 667</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 668">Table 668</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 669">Table 669</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 670">Table 670</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 671">Table 671</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 672">Table 672</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 673">Table 673</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 674">Table 674</a>) <li>Matrix for D2SIG/DPT_T2/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 675">Table 675</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 676">Table 676</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 677">Table 677</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 678">Table 678</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 679">Table 679</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 680">Table 680</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 681">Table 681</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 682">Table 682</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 683">Table 683</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 684">Table 684</a>) <li>Matrix for D2SIG/DABS_Y_T2/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 685">Table 685</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 686">Table 686</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 687">Table 687</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 688">Table 688</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 689">Table 689</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 690">Table 690</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 691">Table 691</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 692">Table 692</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 693">Table 693</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 694">Table 694</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 695">Table 695</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 1st bins of ABS_Y_T2 (<a href="115142?table=Table 696">Table 696</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 697">Table 697</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 698">Table 698</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 699">Table 699</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 700">Table 700</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 701">Table 701</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 702">Table 702</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 703">Table 703</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 704">Table 704</a>) <li>Matrix for D2SIG/DPT_T2/DABS_Y_T2 between the 4th and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 705">Table 705</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 706">Table 706</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 707">Table 707</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 708">Table 708</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 709">Table 709</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 710">Table 710</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 711">Table 711</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 712">Table 712</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 713">Table 713</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 714">Table 714</a>) <li>Matrix for D2SIG/DPT_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 715">Table 715</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 716">Table 716</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 717">Table 717</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 718">Table 718</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 719">Table 719</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 720">Table 720</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 721">Table 721</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 722">Table 722</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 723">Table 723</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 724">Table 724</a>) <li>Matrix for D2SIG/DM_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 725">Table 725</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 726">Table 726</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 727">Table 727</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 728">Table 728</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 729">Table 729</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 730">Table 730</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 731">Table 731</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 732">Table 732</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 733">Table 733</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 734">Table 734</a>) <li>Matrix for D2SIG/DPT_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 735">Table 735</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 736">Table 736</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 737">Table 737</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 738">Table 738</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 739">Table 739</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 740">Table 740</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 741">Table 741</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 742">Table 742</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 743">Table 743</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 744">Table 744</a>) <li>Matrix for D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 745">Table 745</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 746">Table 746</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 747">Table 747</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 748">Table 748</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 749">Table 749</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 750">Table 750</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 751">Table 751</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 752">Table 752</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 753">Table 753</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 754">Table 754</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 755">Table 755</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 756">Table 756</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 757">Table 757</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 758">Table 758</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 759">Table 759</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 760">Table 760</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 761">Table 761</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 762">Table 762</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 763">Table 763</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 764">Table 764</a>) <li>Matrix for D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 765">Table 765</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 1st bins of PT_TTBAR (<a href="115142?table=Table 766">Table 766</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 2nd bins of PT_TTBAR (<a href="115142?table=Table 767">Table 767</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 3rd bins of PT_TTBAR (<a href="115142?table=Table 768">Table 768</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 4th bins of PT_TTBAR (<a href="115142?table=Table 769">Table 769</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 2nd bins of PT_TTBAR (<a href="115142?table=Table 770">Table 770</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 771">Table 771</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 4th bins of PT_TTBAR (<a href="115142?table=Table 772">Table 772</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 773">Table 773</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 4th bins of PT_TTBAR (<a href="115142?table=Table 774">Table 774</a>) <li>Matrix for D2SIG/DM_TTBAR/PT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="115142?table=Table 775">Table 775</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 776">Table 776</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 777">Table 777</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 778">Table 778</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 779">Table 779</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 780">Table 780</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 781">Table 781</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 782">Table 782</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 783">Table 783</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 784">Table 784</a>) <li>Matrix for D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 785">Table 785</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 846">Table 846</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 847">Table 847</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 848">Table 848</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 849">Table 849</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 850">Table 850</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 851">Table 851</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 852">Table 852</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 853">Table 853</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 854">Table 854</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 855">Table 855</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 856">Table 856</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 857">Table 857</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 858">Table 858</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 859">Table 859</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 860">Table 860</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 861">Table 861</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 862">Table 862</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 863">Table 863</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 864">Table 864</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T2/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 865">Table 865</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 866">Table 866</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 867">Table 867</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 868">Table 868</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 869">Table 869</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 870">Table 870</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 871">Table 871</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 872">Table 872</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 873">Table 873</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 874">Table 874</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 875">Table 875</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 1st bins of ABS_Y_T2 (<a href="115142?table=Table 876">Table 876</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 877">Table 877</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 878">Table 878</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 1st and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 879">Table 879</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 2nd bins of ABS_Y_T2 (<a href="115142?table=Table 880">Table 880</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 881">Table 881</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 2nd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 882">Table 882</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 3rd bins of ABS_Y_T2 (<a href="115142?table=Table 883">Table 883</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 3rd and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 884">Table 884</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T2/DABS_Y_T2 between the 4th and 4th bins of ABS_Y_T2 (<a href="115142?table=Table 885">Table 885</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 886">Table 886</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 887">Table 887</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 888">Table 888</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 889">Table 889</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 890">Table 890</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 891">Table 891</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 892">Table 892</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 893">Table 893</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 894">Table 894</a>) <li>Matrix for 1/SIG*D2SIG/DPT_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 895">Table 895</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 1st bins of PT_T1 (<a href="115142?table=Table 896">Table 896</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 2nd bins of PT_T1 (<a href="115142?table=Table 897">Table 897</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 3rd bins of PT_T1 (<a href="115142?table=Table 898">Table 898</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 1st and 4th bins of PT_T1 (<a href="115142?table=Table 899">Table 899</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 2nd bins of PT_T1 (<a href="115142?table=Table 900">Table 900</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 3rd bins of PT_T1 (<a href="115142?table=Table 901">Table 901</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 2nd and 4th bins of PT_T1 (<a href="115142?table=Table 902">Table 902</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 3rd bins of PT_T1 (<a href="115142?table=Table 903">Table 903</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 3rd and 4th bins of PT_T1 (<a href="115142?table=Table 904">Table 904</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DPT_T1 between the 4th and 4th bins of PT_T1 (<a href="115142?table=Table 905">Table 905</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 906">Table 906</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 907">Table 907</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 908">Table 908</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 909">Table 909</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 910">Table 910</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 911">Table 911</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 912">Table 912</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 913">Table 913</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 914">Table 914</a>) <li>Matrix for 1/SIG*D2SIG/DPT_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 915">Table 915</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 916">Table 916</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 917">Table 917</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 918">Table 918</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 919">Table 919</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 920">Table 920</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 921">Table 921</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 922">Table 922</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 923">Table 923</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 924">Table 924</a>) <li>Matrix for 1/SIG*D2SIG/DABS_Y_T1/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 925">Table 925</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 1st bins of ABS_Y_T1 (<a href="115142?table=Table 926">Table 926</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 927">Table 927</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 928">Table 928</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 1st and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 929">Table 929</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 2nd bins of ABS_Y_T1 (<a href="115142?table=Table 930">Table 930</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 931">Table 931</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 2nd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 932">Table 932</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 3rd bins of ABS_Y_T1 (<a href="115142?table=Table 933">Table 933</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 3rd and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 934">Table 934</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_T1 between the 4th and 4th bins of ABS_Y_T1 (<a href="115142?table=Table 935">Table 935</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 936">Table 936</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 937">Table 937</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 938">Table 938</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 939">Table 939</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 940">Table 940</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 941">Table 941</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 942">Table 942</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 943">Table 943</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 944">Table 944</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 945">Table 945</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 1st bins of PT_TTBAR (<a href="115142?table=Table 946">Table 946</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 2nd bins of PT_TTBAR (<a href="115142?table=Table 947">Table 947</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 3rd bins of PT_TTBAR (<a href="115142?table=Table 948">Table 948</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 1st and 4th bins of PT_TTBAR (<a href="115142?table=Table 949">Table 949</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 2nd bins of PT_TTBAR (<a href="115142?table=Table 950">Table 950</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 951">Table 951</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 2nd and 4th bins of PT_TTBAR (<a href="115142?table=Table 952">Table 952</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 3rd bins of PT_TTBAR (<a href="115142?table=Table 953">Table 953</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 3rd and 4th bins of PT_TTBAR (<a href="115142?table=Table 954">Table 954</a>) <li>Matrix for 1/SIG*D2SIG/DM_TTBAR/PT_TTBAR between the 4th and 4th bins of PT_TTBAR (<a href="115142?table=Table 955">Table 955</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 1st bins of ABS_Y_TTBAR (<a href="115142?table=Table 956">Table 956</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 957">Table 957</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 958">Table 958</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 1st and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 959">Table 959</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 2nd bins of ABS_Y_TTBAR (<a href="115142?table=Table 960">Table 960</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 961">Table 961</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 2nd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 962">Table 962</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 3rd bins of ABS_Y_TTBAR (<a href="115142?table=Table 963">Table 963</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 3rd and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 964">Table 964</a>) <li>Matrix for 1/SIG*D2SIG/PT_TTBAR/DABS_Y_TTBAR between the 4th and 4th bins of ABS_Y_TTBAR (<a href="115142?table=Table 965">Table 965</a>) </ul><br/> <u>3D:</u><br/> Spectra: <ul><br/> <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 210">Table 210</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 211">Table 211</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 212">Table 212</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 213">Table 213</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 214">Table 214</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 215">Table 215</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 216">Table 216</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 217">Table 217</a>) <li>D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 218">Table 218</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 282">Table 282</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 283">Table 283</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.0 < ABS_Y_TTBAR < 0.3, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 284">Table 284</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 285">Table 285</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 286">Table 286</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.3 < ABS_Y_TTBAR < 0.9, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 287">Table 287</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 0.9 TeV < M_TTBAR < 1.2 TeV) (<a href="115142?table=Table 288">Table 288</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.2 TeV < M_TTBAR < 1.5 TeV) (<a href="115142?table=Table 289">Table 289</a>) <li>1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR (0.9 < ABS_Y_TTBAR < 2.0, 1.5 TeV < M_TTBAR < 4.0 TeV) (<a href="115142?table=Table 290">Table 290</a>) </ul><br/> Covariances: <ul><br/> <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 786">Table 786</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 787">Table 787</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 788">Table 788</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 789">Table 789</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 790">Table 790</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 791">Table 791</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 792">Table 792</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 793">Table 793</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 794">Table 794</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 795">Table 795</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 796">Table 796</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 797">Table 797</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 798">Table 798</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 799">Table 799</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 800">Table 800</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 801">Table 801</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 802">Table 802</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 803">Table 803</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 804">Table 804</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 805">Table 805</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 806">Table 806</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 807">Table 807</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 808">Table 808</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 809">Table 809</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 810">Table 810</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 811">Table 811</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 812">Table 812</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 813">Table 813</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 814">Table 814</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 815">Table 815</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 816">Table 816</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 817">Table 817</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 818">Table 818</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 819">Table 819</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 820">Table 820</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 821">Table 821</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 822">Table 822</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 823">Table 823</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 824">Table 824</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 825">Table 825</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 826">Table 826</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 827">Table 827</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 828">Table 828</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 829">Table 829</a>) <li>Matrix for D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 830">Table 830</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 966">Table 966</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 967">Table 967</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 968">Table 968</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 969">Table 969</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 970">Table 970</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 971">Table 971</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 972">Table 972</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 973">Table 973</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 974">Table 974</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 975">Table 975</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 976">Table 976</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 977">Table 977</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 978">Table 978</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 979">Table 979</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 980">Table 980</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 981">Table 981</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 982">Table 982</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 983">Table 983</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 984">Table 984</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 985">Table 985</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 986">Table 986</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 987">Table 987</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 988">Table 988</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (1st, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 989">Table 989</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 990">Table 990</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 991">Table 991</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 992">Table 992</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 993">Table 993</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 994">Table 994</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 995">Table 995</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 996">Table 996</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 997">Table 997</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 998">Table 998</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 999">Table 999</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1000">Table 1000</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1001">Table 1001</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1002">Table 1002</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1003">Table 1003</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (2nd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1004">Table 1004</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1005">Table 1005</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1006">Table 1006</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 1st) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1007">Table 1007</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1008">Table 1008</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 2nd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1009">Table 1009</a>) <li>Matrix for 1/SIG*D3SIG/DPT_T1/DABS_Y_TTBAR/DM_TTBAR between the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) and the (3rd, 3rd) bin of (ABS_Y_TTBAR, M_TTBAR) (<a href="115142?table=Table 1010">Table 1010</a>) </ul><br/>
Fiducial phase-space cross-section at particle level.
$p_{T}^{t}$ absolute differential cross-section at particle level.
A search for Higgs boson decays into a $Z$ boson and a light resonance in two-lepton plus jet events is performed, using a $pp$ collision dataset with an integrated luminosity of 139 fb$^{-1}$ collected at $\sqrt{s}=13$ TeV by the ATLAS experiment at the CERN LHC. The resonance considered is a light boson with a mass below 4 GeV from a possible extended scalar sector, or a charmonium state. Multivariate discriminants are used for the event selection and for evaluating the mass of the light resonance. No excess of events above the expected background is found. Observed (expected) 95$\% $ confidence-level upper limits are set on the Higgs boson production cross section times branching fraction to a $Z$ boson and the signal resonance, with values in the range 17 pb to 340 pb ($16^{+6}_{-5}$ pb to $320^{+130}_{-90}$ pb) for the different light spin-0 boson mass and branching fraction hypotheses, and with values of 110 pb and 100 pb ($100^{+40}_{-30}$ pb and $100^{+40}_{-30}$ pb) for the $\eta_c$ and $J/\psi$ hypotheses, respectively.
Observed number of data events and expected number of background events in the signal region.
Efficiencies of the MLP selection, complete selection and total expected signal yields for each signal sample, assuming B$(H\to Z(Q/a))=100\%$ and $\sigma(pp\to H) = \sigma_\text{SM}(pp\to H)$. Pythia 8 branching fractions of $a$ are assumed using a $\tan\beta$ value of 1. The MLP efficiencies, total efficiencies, and expected yields are determined using MC samples, with uncertainties due to MC sample statistics, except for the expected background yield. The expected background yield and its uncertainty is calculated as described in the main text of the paper.
Expected and observed 95% CL upper limits on $\sigma(pp\to H)B(H\to Za)/$pb. These results are quoted for $B(a\to gg)=100\%$ and $B(a\to s\bar{s})=100\%$ for each signal sample. The smaller (larger) quoted ranges around the expected limits represent $\pm 1\sigma$ ($\pm 2\sigma$) fluctuations.
A search for the $Z\gamma$ decay of the Higgs boson, with $Z$ boson decays into pairs of electrons or muons is presented. The analysis uses proton$-$proton collision data at $\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 139 fb$^{-1}$ recorded by the ATLAS detector at the Large Hadron Collider. The observed data are consistent with the expected background with a $p$-value of 1.3%. An upper limit at 95% confidence level on the production cross-section times the branching ratio for $pp\to H\to Z\gamma$ is set at 3.6 times the Standard Model prediction while 2.6 times is expected in the presence of the Standard Model Higgs boson. The best-fit value for the signal yield normalised to the Standard Model prediction is $2.0^{+1.0}_{-0.9}$ where the statistical component of the uncertainty is dominant.
The number of data events selected in each category, and in the $Z\gamma$ mass range of 105--160 GeV. In addition, the following numbers are given: the expected number of Higgs boson signal events in an interval around the peak position for a signal of $m_{H}=125.09$ GeV containing 68% of the SM signal ($S_{68}$), the mass resolution quantified by the width of the $S_{68}$ interval ($w_{68}$) defined by the difference between the 84th and the 16th percentile of the signal mass distribution, the background in the $S_{68}$ interval ($B_{68}$) is estimated from fits to the data using the background models described in paper, the observed number of events in the $S_{68}$ interval ($N_{68}$), the expected signal-to-background ratio in the $S_{68}$ window ($S_{68}/B_{68}$), and the expected significance estimate defined as $S_{68}/\sqrt{S_{68}+B_{68}}$. The final row of the table displays the expected number of events for an analysis performed in a single inclusive category.
Upper limit at 95% confidence level on the signal yield normalised to the Standard Model prediction (signal strength) for $pp \to H \to Z+\gamma$
The best fit value for the signal yield normalised to the Standard Model prediction (signal strength) for $pp \to H \to Z+\gamma$
A search is presented for new phenomena in events characterised by high jet multiplicity, no leptons (electrons or muons), and four or more jets originating from the fragmentation of $b$-quarks ($b$-jets). The search uses 139 fb$^{-1}$ of $\sqrt{s}$ = 13 TeV proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider during Run 2. The dominant Standard Model background originates from multijet production and is estimated using a data-driven technique based on an extrapolation from events with low $b$-jet multiplicity to the high $b$-jet multiplicities used in the search. No significant excess over the Standard Model expectation is observed and 95% confidence-level limits that constrain simplified models of R-parity-violating supersymmetry are determined. The exclusion limits reach 950 GeV in top-squark mass in the models considered.
<b>- - - - - - - - Overview of HEPData Record - - - - - - - -</b> <br><br> <b>Exclusion contours:</b> <ul> <li><a href="?table=stbchionly_obs">Stop to bottom quark and chargino exclusion contour (Obs.)</a> <li><a href="?table=stbchionly_exp">Stop to bottom quark and chargino exclusion contour (Exp.)</a> <li><a href="?table=stbchi_obs">Stop to higgsino LSP exclusion contour (Obs.)</a> <li><a href="?table=stbchi_exp">Stop to higgsino LSP exclusion contour (Exp.)</a> <li><a href="?table=sttN_obs">Stop to top quark and neutralino exclusion contour (Obs.)</a> <li><a href="?table=sttN_exp">Stop to top quark and neutralino exclusion contour (Exp.)</a> </ul> <b>Upper limits:</b> <ul> <li><a href="?table=stbchionly_xSecUL_obs">Obs Xsection upper limit in stop to bottom quark and chargino</a> <li><a href="?table=stop_xSecUL_obs">Obs Xsection upper limit in higgsino LSP</a> <li><a href="?table=stbchionly_xSecUL_exp">Exp Xsection upper limit in stop to bottom quark and chargino</a> <li><a href="?table=stop_xSecUL_exp">Exp Xsection upper limit in higgsino LSP</a> </ul> <b>Kinematic distributions:</b> <ul> <li><a href="?table=SR_yields">SR_yields</a> </ul> <b>Cut flows:</b> <ul> <li><a href="?table=cutflow">cutflow</a> </ul> <b>Acceptance and efficiencies:</b> As explained in <a href="https://twiki.cern.ch/twiki/bin/view/AtlasPublic/SupersymmetryPublicResults#summary_of_auxiliary_material">the twiki</a>. <ul> <li> <b>stbchi_6je4be:</b> <a href="?table=stbchi_Acc_6je4be">stbchi_Acc_6je4be</a> <a href="?table=stbchi_Eff_6je4be">stbchi_Eff_6je4be</a> <li> <b>stbchi_7je4be:</b> <a href="?table=stbchi_Acc_7je4be">stbchi_Acc_7je4be</a> <a href="?table=stbchi_Eff_7je4be">stbchi_Eff_7je4be</a> <li> <b>stbchi_8je4be:</b> <a href="?table=stbchi_Acc_8je4be">stbchi_Acc_8je4be</a> <a href="?table=stbchi_Eff_8je4be">stbchi_Eff_8je4be</a> <li> <b>stbchi_9ji4be:</b> <a href="?table=stbchi_Acc_9ji4be">stbchi_Acc_9ji4be</a> <a href="?table=stbchi_Eff_9ji4be">stbchi_Eff_9ji4be</a> <li> <b>stbchi_6je5bi:</b> <a href="?table=stbchi_Acc_6je5bi">stbchi_Acc_6je5bi</a> <a href="?table=stbchi_Eff_6je5bi">stbchi_Eff_6je5bi</a> <li> <b>stbchi_7je5bi:</b> <a href="?table=stbchi_Acc_7je5bi">stbchi_Acc_7je5bi</a> <a href="?table=stbchi_Eff_7je5bi">stbchi_Eff_7je5bi</a> <li> <b>stbchi_8je5bi:</b> <a href="?table=stbchi_Acc_8je5bi">stbchi_Acc_8je5bi</a> <a href="?table=stbchi_Eff_8je5bi">stbchi_Eff_8je5bi</a> <li> <b>stbchi_9ji5bi:</b> <a href="?table=stbchi_Acc_9ji5bi">stbchi_Acc_9ji5bi</a> <a href="?table=stbchi_Eff_9ji5bi">stbchi_Eff_9ji5bi</a> <li> <b>stbchi_8ji5bi:</b> <a href="?table=stbchi_Acc_8ji5bi">stbchi_Acc_8ji5bi</a> <a href="?table=stbchi_Eff_8ji5bi">stbchi_Eff_8ji5bi</a> <li> <b>sttN_6je4be:</b> <a href="?table=sttN_Acc_6je4be">sttN_Acc_6je4be</a> <a href="?table=sttN_Eff_6je4be">sttN_Eff_6je4be</a> <li> <b>sttN_7je4be:</b> <a href="?table=sttN_Acc_7je4be">sttN_Acc_7je4be</a> <a href="?table=sttN_Eff_7je4be">sttN_Eff_7je4be</a> <li> <b>sttN_8je4be:</b> <a href="?table=sttN_Acc_8je4be">sttN_Acc_8je4be</a> <a href="?table=sttN_Eff_8je4be">sttN_Eff_8je4be</a> <li> <b>sttN_9ji4be:</b> <a href="?table=sttN_Acc_9ji4be">sttN_Acc_9ji4be</a> <a href="?table=sttN_Eff_9ji4be">sttN_Eff_9ji4be</a> <li> <b>sttN_6je5bi:</b> <a href="?table=sttN_Acc_6je5bi">sttN_Acc_6je5bi</a> <a href="?table=sttN_Eff_6je5bi">sttN_Eff_6je5bi</a> <li> <b>sttN_7je5bi:</b> <a href="?table=sttN_Acc_7je5bi">sttN_Acc_7je5bi</a> <a href="?table=sttN_Eff_7je5bi">sttN_Eff_7je5bi</a> <li> <b>sttN_8je5bi:</b> <a href="?table=sttN_Acc_8je5bi">sttN_Acc_8je5bi</a> <a href="?table=sttN_Eff_8je5bi">sttN_Eff_8je5bi</a> <li> <b>sttN_9ji5bi:</b> <a href="?table=sttN_Acc_9ji5bi">sttN_Acc_9ji5bi</a> <a href="?table=sttN_Eff_9ji5bi">sttN_Eff_9ji5bi</a> <li> <b>sttN_8ji5bi:</b> <a href="?table=sttN_Acc_8ji5bi">sttN_Acc_8ji5bi</a> <a href="?table=sttN_Eff_8ji5bi">sttN_Eff_8ji5bi</a> </ul> <b>Truth Code snippets</b> and <b>SLHA</a> files are available under "Resources" (purple button on the left)
The observed exclusion contour at 95% CL as a function of the $\it{m}_{\tilde{\chi}^{\pm}_{1}}$ vs. $\it{m}_{\tilde{t}}$. Masses that are within the contours are excluded. Limits are shown for $B(\tilde{t} \rightarrow b \chi^{+}_{1})$ equal to unity.
The expected exclusion contour at 95% CL as a function of the $\it{m}_{\tilde{\chi}^{\pm}_{1}}$ vs. $\it{m}_{\tilde{t}}$. Masses that are within the contour are excluded. Limits are shown for $B(\tilde{t} \rightarrow b \chi^{+}_{1})$ equal to unity.
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 pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark, is presented. This is the first leptoquark search using ATLAS data to investigate top-philic cross-generational couplings that could provide explanations for recently observed anomalies in $B$ meson decays. This analysis targets high leptoquark masses which cause the decay products of each resultant top quark to be contained within a single high-$p_{\mathrm{T}}$ large-radius jet. The full Run 2 dataset is exploited, consisting of 139 fb$^{-1}$ of data collected from proton-proton collisions at $\sqrt{s}=13$ TeV from 2015 to 2018 with the ATLAS detector at the CERN Large Hadron Collider. In the absence of any significant deviation from the background expectation, lower limits on the leptoquark masses are set at 1480 GeV and 1470 GeV for the electron and muon channel, respectively.
Expected and observed upper limits at the 95% CL on the leptoquark pair production cross section as a function of leptoquark mass under the assumption of $\mathcal{B}$(LQ->$te$)=1.
Expected and observed upper limits at the 95% CL on the leptoquark pair production cross section as a function of leptoquark mass under the assumption of $\mathcal{B}$(LQ->$t\mu$)=1.
Expected and observed 95% CL lower limits on the leptoquark mass as a function of the branching ratio $\mathcal{B}$(LQ->$te$).
Higgs boson properties are studied in the four-lepton decay channel (where lepton = $e$, $\mu$) using 139 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}$ = 13 TeV by the ATLAS experiment at the Large Hadron Collider. The inclusive cross-section times branching ratio for $H\to ZZ^*$ decay is measured to be $1.34 \pm 0.12$ pb for a Higgs boson with absolute rapidity below 2.5, in good agreement with the Standard Model prediction of $1.33 \pm 0.08$ pb. Cross-sections times branching ratio are measured for the main Higgs boson production modes in several exclusive phase-space regions. The measurements are interpreted in terms of coupling modifiers and of the tensor structure of Higgs boson interactions using an effective field theory approach. Exclusion limits are set on the CP-even and CP-odd `beyond the Standard Model' couplings of the Higgs boson to vector bosons, gluons and top quarks.
The expected number of SM Higgs boson events with a mass $m_{H}$= 125 GeV for an integrated luminosity of 139 fb$^{-1}$ at $\sqrt{s}$=13 TeV in each reconstructed event signal (115 < $m_{4l}$< 130 GeV) and sideband ($m_{4l}$ in 105-115 GeV or 130-160 GeV for $ZZ^{*}$, 130-350 GeV for $tXX$) category, shown separately for each production bin of the Production Mode Stage. The ggF and $bbH$ yields are shown separately but both contribute to the same (ggF)production bin, and $ZH$ and $WH$ are reported separately but are merged together for the final result. Statistical and systematic uncertainties, including those for total SM cross-section predictions, are added in quadrature. Contributions that are below 0.2% of the total signal in each reconstructed event category are not shown and are replaced by -.
The impact of the dominant systematic uncertainties (in percent) on the cross-sections in production bins of the Production Mode Stage and the Reduced Stage 1.1. Similar sources of systematic uncertainties are grouped together in luminosity (Lumi.),electron/muon reconstruction and identification efficiencies and pile up modelling ($e$, $\mu$, pile up), jet energy scale/resolution and $b$-tagging efficiencies (Jets, flav. tag), uncertainties in reducible background (reducible bkg), theoretical uncertainties in $ZZ^{*}$ background and $tXX$ background, and theoretical uncertainties in the signal due to parton distribution function (PDF), QCD scale (QCD) and parton showering algorithm (Shower). The uncertainties are rounded to the nearest 0.5%, except for the luminosity uncertainty, which is measured to be 1.7% and increases for the $VH$ signal processes due to the simulation-based normalisation of the $VVV$ background. The uncertainties that are below 0.5% are not shown and replaced by -.
The expected and the observed (post-fit) the four-lepton invariant mass distribution for the selected Higgs boson candidates, shown for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed tohave a mass $m_{H}$= 125GeV.
Inclusive and differential fiducial cross sections of the Higgs boson are measured in the $H \to ZZ^{*} \to 4\ell$ ($\ell = e,\mu$) decay channel. The results are based on proton$-$proton collision data produced at the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector from 2015 to 2018, equivalent to an integrated luminosity of 139 fb$^{-1}$. The inclusive fiducial cross section for the $H \to ZZ^{*} \to 4\ell$ process is measured to be $\sigma_\mathrm{fid} = 3.28 \pm 0.32$ fb, in agreement with the Standard Model prediction of $\sigma_\mathrm{fid, SM} = 3.41 \pm 0.18 $ fb. Differential fiducial cross sections are measured for a variety of observables which are sensitive to the production and decay of the Higgs boson. All measurements are in agreement with the Standard Model predictions. The results are used to constrain anomalous Higgs boson interactions with Standard Model particles.
Fractional uncertainties for the inclusive fiducial and total cross sections, and range of systematic uncertainties for the differential measurements. The columns e/$\mu$ and jets represent the experimental uncertainties in lepton and jet reconstruction and identification, respectively. The Z + jets, $t\bar{t}$, tXX (Other Bkg.) column includes uncertainties related to the estimation of these background sources. The $ZZ^{*}$ theory ($ZZ^{*}$ th.) uncertainties include the PDF and scale variations. Signal theory (Sig th.) uncertainties include PDF choice, QCD scale, and shower modelling of the signal. Finally, the column labelled Comp. contains uncertainties related to production mode composition and unfolding bias which affect the response matrices. The uncertainties have been rounded to the nearest 0.5%, except for the luminosity uncertainty which has been measured to be 1.7%.
Expected (pre-fit) and observed number of events in the four decay final states after the event selection, in the mass range 115< $m_{4l}$ < 130 GeV. The sum of the expected number of SM Higgs boson events and the estimated background yields is compared to the data. Combined statistical and systematic uncertainties are included for the predictions.
The fiducial and total cross sections of Higgs boson production measured in the 4l final state. The fiducial cross sections are given separately for each decay final state, and for same- and different-flavour decays. The inclusive fiducial cross section is measured as the sum of all final states ($\sigma_{sum}$), as well as by combining the per-final state measurements assuming SM $ZZ^{*} \to 4l$ relative branching ratios ($\sigma_{comb}$). For the total cross section ($\sigma_{tot}$), the Higgs boson branching ratio at $m_{H}$= 125 GeV is assumed. The total SM prediction is accurate to N3LO in QCD and NLO EW for the ggF process. The cross sections for all other Higgs boson production modes XH are added. For the fiducial cross section predictions, the SM cross sections are multiplied by the acceptances determined using the NNLOPS sample for ggF. The p-values indicating the compatibility of the measurement and the SM prediction are shown as well. They do not include the systematic uncertainty in the theoretical predictions.
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