We report the result of a brief experiment to measure the cross section for photoproduction of Jψ(3100). At a mean energy of 55 GeV we find this cross section per nucleon to be 37.5 ± 8.2 (statistical) ± 4 (systematic) nb. The result establishes the previously indicated rise in Jψ photoproduction on protons above 20 GeV and suggests that the rise has occurred by 55 GeV.
Final total cross sections are given for a counter experiment at SLAC on hadronic photon absorption in hydrogen, deuterium, carbon, copper, and lead at incident energies from 3.7 to 18.3 GeV. Some of the nucleon cross sections have been revised and the C, Cu, and Pb data from 3.7 to 7.4 GeV have not been reported previously. The cross sections for complex nuclei vary approximately as A0.9 in our energy range, indicating that the photon interacts, at least partially, as a strongly interacting particle. The energy dependences of the proton and neutron cross sections are also similar to those of hadron-nucleon cross sections and hence may be fitted by a typical Regge parametrization, yielding σT(γp)=(98.7±3.6)+(65.0±10.1)ν−12 μb and σT(γn)=(103.4±6.7)+(33.1±19.4)ν−12 μb, where ν is the photon energy in GeV. These extrapolate to the same value at infinite energy, consistent with Pomeranchukon exchange, and the energy-dependent part yields an isovector-to-isoscalar-exchange ratio of 0.18 ± 0.06. While these observations are qualitatively consistent with vector meson dominance, quantitatively vector dominance fails in relating our results to ρ photo-production on hydrogen or to experiments determining the ρ-nucleon cross section. Vector dominance cannot be rescued by assuming that the ρ-photon coupling constant depends on the photon mass. Instead, an additional short-range interaction is apparently required, possibly due to a heavy (≳ 2 GeV / c2) vector meson or to a bare-photon interaction. The additional interaction accounts for approximately 20% of the total photoabsorption cross section.
The fragmentation properties of jets containing $b$-hadrons are studied using charged $B$ mesons in 139 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV, recorded with the ATLAS detector at the LHC during the period from 2015 to 2018. The $B$ mesons are reconstructed using the decay of $B^{\pm}$ into $J/\psi K^{\pm}$, with the $J/\psi$ decaying into a pair of muons. Jets are reconstructed using the anti-$k_t$ algorithm with radius parameter $R=0.4$. The measurement determines the longitudinal and transverse momentum profiles of the reconstructed $B$ hadrons with respect to the axes of the jets to which they are geometrically associated. These distributions are measured in intervals of the jet transverse momentum, ranging from 50 GeV to above 100 GeV. The results are corrected for detector effects and compared with several Monte Carlo predictions using different parton shower and hadronisation models. The results for the longitudinal and transverse profiles provide useful inputs to improve the description of heavy-flavour fragmentation in jets.
A partial wave analysis of the centrally produced eta pi0 and eta pi- channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. Clear a0(980) and a2(1320) signals have been observed in S and D+ waves respectively. The dPT, phi and |t| distributions of these resonances are presented.
A direct search for Higgs bosons produced via vector-boson fusion and subsequently decaying into invisible particles is reported. The analysis uses 139 $\text{fb}^{-1}$ of $pp$ collision data at a centre-of-mass energy of $\sqrt{s}$=13 $\text{TeV}$ recorded by the ATLAS detector at the LHC. The observed numbers of events are found to be in agreement with the background expectation from Standard Model processes. For a scalar Higgs boson with a mass of 125 $\text{GeV}$ and a Standard Model production cross section, an observed upper limit of $0.145$ is placed on the branching fraction of its decay into invisible particles at 95% confidence level, with an expected limit of $0.103$. These results are interpreted in the context of models where the Higgs boson acts as a portal to dark matter, and limits are set on the scattering cross section of weakly interacting massive particles and nucleons. Invisible decays of additional scalar bosons with masses from 50 $\text{GeV}$ to 2 $\text{TeV}$ are also studied, and the derived upper limits on the cross section times branching fraction decrease with increasing mass from 1.0 $\text{pb}$ for a scalar boson mass of 50 $\text{GeV}$ to 0.1 $\text{pb}$ at a mass of 2 $\text{TeV}$.
The reaction pp→p f ( π + π − π + π − )p s , where the π + π − π + π − system is centrally produced, has been studied at 300 GeV/ c in an experiment designed to search for gluonic states. The π + π − π + π − mass spectrum shows evidence for the f 1 (1285) with a mass of 1281±1 MeV and a width of 31±5 MeV. In addition there is evidence for two new enhancements at masses of 1449±4 and 1901±13 MeV with widths of 78±18 and 312±61 MeV respectively. An analysis of the state at 1.45 GeV indicates that it is not a π + π − π + π − decay mode of the f 1 (1420) or ι η(1440) .
We report a measurement of the forward-backward asymmetry, $A_{FB}$, in $b\bar{b}$ pairs produced in proton-antiproton collisions and identified by muons from semileptonic $b$-hadron decays. The event sample was collected at a center-of-mass energy of $\sqrt{s}=1.96$ TeV with the CDF II detector and corresponds to 6.9 fb$^{-1}$ of integrated luminosity. We obtain an integrated asymmetry of $A_{FB}(b\bar{b})=(1.2 \pm 0.7)$\% at the particle level for $b$-quark pairs with invariant mass, $m_{b\bar{b}}$, down to $40$ GeV/$c^2$ and measure the dependence of $A_{FB}(b\bar{b})$ on $m_{b\bar{b}}$. The results are compatible with expectations from the standard model.
The structure function F2γ for a quasireal photon has been measured in the reaction ee→eeX for Q2 in the range 0.2<Q2<7 GeV2, by use of 9200 multihadron events obtained with the TPC/Two-Gamma detector at the SLAC storage ring PEP. The data have been corrected for detector effects by a regularized unfolding procedure and are presented as F2γ(x,Q2). The structure function shows scaling in the region 0.3<Q2<1.6 GeV2, x<0.3, and rises for higher Q2 and x>0.1. Below Q2=0.3 GeV2, scaling breaks down in accordance with the finite cross-section bound for real photons.
At the Fermilab Tevatron proton-antiproton ($p\bar{p}$) collider, Drell-Yan lepton pairs are produced in the process $p \bar{p} \rightarrow e^+e^- + X$ through an intermediate $\gamma^*/Z$ boson. The forward-backward asymmetry in the polar-angle distribution of the $e^-$ as a function of the $e^+e^-$-pair mass is used to obtain $\sin^2\theta^{\rm lept}_{\rm eff}$, the effective leptonic determination of the electroweak-mixing parameter $\sin^2\theta_W$. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.4~fb$^{-1}$ of integrated luminosity from $p\bar{p}$ collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II data set. The value of $\sin^2\theta^{\rm lept}_{\rm eff}$ is found to be $0.23248 \pm 0.00053$. The combination with the previous CDF measurement based on $\mu^+\mu^-$ pairs yields $\sin^2\theta^{\rm lept}_{\rm eff} = 0.23221 \pm 0.00046$. This result, when interpreted within the specified context of the standard model assuming $\sin^2 \theta_W = 1 - M_W^2/M_Z^2$ and that the $W$- and $Z$-boson masses are on-shell, yields $\sin^2\theta_W = 0.22400 \pm 0.00045$, or equivalently a $W$-boson mass of $80.328 \pm 0.024 \;{\rm GeV}/c^2$.
A search for Majorana neutrinos in same-sign $WW$ scattering events is presented. The analysis uses $\sqrt{s}= 13$ TeV proton-proton collision data with an integrated luminosity of 140 fb$^{-1}$ recorded during 2015-2018 by the ATLAS detector at the Large Hadron Collider. The analysis targets final states including exactly two same-sign muons and at least two hadronic jets well separated in rapidity. The modelling of the main backgrounds, from Standard Model same-sign $WW$ scattering and $WZ$ production, is constrained with data in dedicated signal-depleted control regions. The distribution of the transverse momentum of the second-hardest muon is used to search for signals originating from a heavy Majorana neutrino with a mass between 50 GeV and 20 TeV. No significant excess is observed over the background expectation. The results are interpreted in a benchmark scenario of the Phenomenological Type-I Seesaw model. In addition, the sensitivity to the Weinberg operator is investigated. Upper limits at the 95% confidence level are placed on the squared muon-neutrino-heavy-neutrino mass-mixing matrix element $\vert V_{\mu N} \vert^{2}$ as a function of the heavy Majorana neutrino's mass $m_N$, and on the effective $\mu\mu$ Majorana neutrino mass $|m_{\mu\mu}|$.
The π−+p→π0+n differential cross section at 180° has been measured for 52 values of π− momentum from 1.8 to 6.0 GeV/c using a constant-geometry detection system. The average statistical uncertainty is ∼5% and the systematic uncertainty is ∼10%. The details of the experiment and the data analysis are discussed. The data are compared with those of other experiments with which they are generally in agreement. One set of data disagrees with those presented here and a possible reason for this is discussed. A five-parameter fit of the predictions of a dual-resonance model to our data gave excellent agreement. The differential cross sections at 180° for π±p elastic scattering have been compiled and the moduli and relative phase of the T=12 and T=32 pion-nucleon s- and u-channel amplitudes (|A12|, |A32|, and cosδ) have a minimum at u=0.4 GeV/c and, in the s channel, a corresponding minimum at s=2.2 GeV/c.
No description provided.
The differential cross sections for π−p elastic scattering over the angular range 155° to 177° in the center of mass have been measured at 33 incident-pion momenta in the range 600 to 1280 MeV/c. Angular distributions are presented. The extrapolated differential cross sections at 180° show considerable structure, in particular a dip near 1150 MeV/c. In general the near-180° cross sections do not agree with existing phase shift solutions above 1000 MeV/c
No description provided.
Differential cross sections for π−p elastic scattering over the angular range 155° to 177° in the center-of-mass system have been measured at 33 incident pion momenta in the range 600 to 1280 MeV/c. The experiment, which was performed at the Bevatron at the Lawrence Berkeley Laboratory, employed a liquid hydrogen target, a double-arm spectrometer, and standard counter techniques to detect the elastic events. The data from this experiment are compared to all other published data in this momentum region. The over-all agreement is good. The data of this experiment are also compared with the results of the recent phase-shift analysis by Almehed and Lovelace. In the momentum region between 700 and 900 MeV/c, the slope of the backward angular distribution goes rapidly through zero from negative to positive, and the magnitude of the differential cross section falls by more than a factor of 10. Momentum-dependent structure is seen in the extrapolated differential cross sections at 180°. Two prominent dips in the 180° differential cross sections appear at 880 and 1150 MeV/c. This structure is discussed in terms of a direct-channel resonance model that assumes only resonant partial waves are contributing to the cross sections for large scattering angles.
No description provided.
Searches are conducted for new spin-0 or spin-1 bosons using events where a Higgs boson with mass $125$ GeV decays into four leptons ($\ell =$$e$,$\mu$). This decay is presumed to occur via an intermediate state which contains two on-shell, promptly decaying bosons: $H \rightarrow XX/ZX \rightarrow 4\ell$, where the new boson $X$ has a mass between 1 and 60 GeV. The search uses $pp$ collision data collected with the ATLAS detector at the LHC with an integrated luminosity of 139 fb$^{-1}$ at a centre-of-mass energy $\sqrt{s}=13$ TeV. The data are found to be consistent with Standard Model expectations. Limits are set on fiducial cross sections and on the branching ratio of the Higgs boson to decay into $XX/ZX$, improving those from previous publications by a factor between two and four. Limits are also set on mixing parameters relevant in extensions of the Standard Model containing a dark sector where $X$ is interpreted to be a dark boson.
Observed and expected upper limits at 95% CL for the cross section of the $H\to Z_dZ_d\to 4\ell$ process, assuming SM Higgs boson production via the gluon-gluon fusion process. All final states are combined.
Observed and expected upper limits at 95% CL for the cross sections of the $H\to Z_dZ_d\to 4\mu$ processes, assuming SM Higgs boson production via the gluon-gluon fusion process. The regions of 2 GeV to 4.4 GeV, and 8 GeV to 12 GeV are each excluded by the quarkonia veto. The step changes at $m_{Z_d}= 15 \,\text{GeV}$ are due to the change in selection from the Low Mass to the High Mass analysis.
Observed and expected upper limits at 95% CL for the cross sections of the $H\to aa\to 4\mu$ processes, assuming SM Higgs boson production via the gluon-gluon fusion process. The regions of 2 GeV to 4.4 GeV, and 8 GeV to 12 GeV are each excluded by the quarkonia veto. The step changes at $m_{Z_d}= 15 \,\text{GeV}$ are due to the change in selection from the Low Mass to the High Mass analysis.
We present a measurement of the total cross section for γγ→hadrons, with one photon quasireal and the other a spacelike photon of mass squared −Q2. Results are presented as a function of Q2 and the γγ center-of-mass energy W, with the Q2 range extending from 0.2 to 60 GeV2, and W in the range from 2 to 10 GeV. The data were taken with the TPC/Two-Gamma facility at the SLAC e+e− storage ring PEP, which was operated at a beam energy of 14.5 GeV. The cross section exhibits a gentle falloff with increasing W. Its Q2 dependence is shown to be well described by an incoherent sum of vector-meson and pointlike scattering over most of the observed W range. Agreement at high Q2 is improved if a minimum-pT cutoff (motivated by QCD) is imposed on the pointlike contribution.
A search for events with two displaced vertices from long-lived particles (LLP) pairs using data collected by the ATLAS detector at the LHC is presented. This analysis uses 139~fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV recorded in 2015-2018. The search employs techniques for reconstructing vertices of LLPs decaying to jets in the muon spectrometer displaced between 3 m and 14 m with respect to the primary interaction vertex. The observed numbers of events are consistent with the expected background and limits for several benchmark signals are determined. For the Higgs boson with a mass of 125 GeV, the paper reports the first exclusion limits for branching fractions into neutral long-lived particles below 0.1%, while branching fractions above 10% are excluded at 95% confidence level for LLP proper lifetimes ranging from 4 cm to 72.4 m. In addition, the paper present the first results for the decay of LLPs into into $t\bar{t}$ in the ATLAS muon spectrometer.
A search for diphoton resonances in the mass range between 10 and 70 GeV with the ATLAS experiment at the Large Hadron Collider (LHC) is presented. The analysis is based on $pp$ collision data corresponding to an integrated luminosity of 138 fb$^{-1}$ at a centre-of-mass energy of 13 TeV recorded from 2015 to 2018. Previous searches for diphoton resonances at the LHC have explored masses down to 65 GeV, finding no evidence of new particles. This search exploits the particular kinematics of events with pairs of closely spaced photons reconstructed in the detector, allowing examination of invariant masses down to 10 GeV. The presented strategy covers a region previously unexplored at hadron colliders because of the experimental challenges of recording low-energy photons and estimating the backgrounds. No significant excess is observed and the reported limits provide the strongest bound on promptly decaying axion-like particles coupling to gluons and photons for masses between 10 and 70 GeV.
A novel search for exotic decays of the Higgs boson into pairs of long-lived neutral particles, each decaying into a bottom quark pair, is performed using 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data collected with the ATLAS detector at the LHC. Events consistent with the production of a Higgs boson in association with a leptonically decaying $Z$ boson are analysed. Long-lived particle (LLP) decays are reconstructed from inner-detector tracks as displaced vertices with high mass and track multiplicity relative to Standard Model processes. The analysis selection requires the presence of at least two displaced vertices, effectively suppressing Standard Model backgrounds. The residual background contribution is estimated using a data-driven technique. No excess over Standard Model predictions is observed, and upper limits are set on the branching ratio of the Higgs boson to LLPs. Branching ratios above 10% are excluded at 95% confidence level for LLP mean proper lifetimes $c\tau$ as small as 4 mm and as large as 100 mm. For LLP masses below 40 GeV, these results represent the most stringent constraint in this lifetime regime.
We measure the ratio of cross section times branching fraction, $R_p \equiv \sigma_{\chi_{c2}} {\cal B}(\chi_{c2} \to J/\psi \gamma)/ \sigma_{\chi_{c1}} {\cal B}(\chi_{c1} \to J/\psi \gamma)$, in 1.1 fb$^{-1}$ of $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96 TeV. This measurement covers the kinematic range $p_T(J/\psi)>4.0$ GeV/$c$, $|\eta(J/\psi)| < 1.0$, and $p_T(\gamma)>1.0$ GeV/$c$. For events due to prompt processes, we find $R_p = 0.395\pm0.016(stat.)\pm0.015(sys.)$. This result represents a significant improvement in precision over previous measurements of prompt $\chi_{c1,2}$ hadroproduction.
A search for charginos and neutralinos at the Large Hadron Collider is reported using fully hadronic final states and missing transverse momentum. Pair-produced charginos or neutralinos are explored, each decaying into a high-$p_{\text{T}}$ Standard Model weak boson. Fully-hadronic final states are studied to exploit the advantage of the large branching ratio, and the efficient background rejection by identifying the high-$p_{\text{T}}$ bosons using large-radius jets and jet substructure information. An integrated luminosity of 139 fb$^{-1}$ of proton-proton collision data collected by the ATLAS detector at a center-of-mass energy of 13 TeV is used. No significant excess is found beyond the Standard Model expectation. The 95% confidence level exclusion limits are set on wino or higgsino production with varying assumptions in the decay branching ratios and the type of the lightest supersymmetric particle. A wino (higgsino) mass up to 1060 (900) GeV is excluded when the lightest SUSY particle mass is below 400 (240) GeV and the mass splitting is larger than 400 (450) GeV. The sensitivity to high-mass wino and higgsino is significantly extended compared with the previous LHC searches using the other final states.
We present a measurement of the $\ttbar$ differential cross section with respect to the $\ttbar$ invariant mass, dSigma/dMttbar, in $\ppbar$ collisions at $\sqrt{s}=1.96$ TeV using an integrated luminosity of $2.7\invfb$ collected by the CDF II experiment. The $\ttbar$ invariant mass spectrum is sensitive to a variety of exotic particles decaying into $\ttbar$ pairs. The result is consistent with the standard model expectation, as modeled by \texttt{PYTHIA} with \texttt{CTEQ5L} parton distribution functions.
A search for supersymmetry involving the pair production of gluinos decaying via off-shell third-generation squarks into the lightest neutralino ($\tilde\chi^0_1$) is reported. It exploits LHC proton$-$proton collision data at a centre-of-mass energy $\sqrt{s} = 13$ TeV with an integrated luminosity of 139 fb$^{-1}$ collected with the ATLAS detector from 2015 to 2018. The search uses events containing large missing transverse momentum, up to one electron or muon, and several energetic jets, at least three of which must be identified as containing $b$-hadrons. Both a simple kinematic event selection and an event selection based upon a deep neural-network are used. No significant excess above the predicted background is found. In simplified models involving the pair production of gluinos that decay via off-shell top (bottom) squarks, gluino masses less than 2.44 TeV (2.35 TeV) are excluded at 95% CL for a massless $\tilde\chi^0_1$. Limits are also set on the gluino mass in models with variable branching ratios for gluino decays to $b\bar{b}\tilde\chi^0_1$, $t\bar{t}\tilde\chi^0_1$ and $t\bar{b}\tilde\chi^-_1$ / $\bar{t}b\tilde\chi^+_1$.
The results of a study of the annihilation reactions n p → θπ + and n p → ωπ + are reported; the data were collected by the OBELIX apparatus, with antineutrons annihilating in flight (momenta from ∼ 50 MeV/ c to 405 MeV/ c ). Annihilation frequencies and annihilation cross sections have been deduced, for both channels, as a function of antineutron momentum. From the cross section ratio, a substantial deviation from OZI rule expectations is observed. An s s quark content in the nucleon offers a fairly plausible explanation for such an effect.
A search for new phenomena has been performed in final states with at least one isolated high-momentum photon, jets and missing transverse momentum in proton--proton collisions at a centre-of-mass energy of $\sqrt{s} = 13$ TeV. The data, collected by the ATLAS experiment at the CERN LHC, correspond to an integrated luminosity of 139 $fb^{-1}$. The experimental results are interpreted in a supersymmetric model in which pair-produced gluinos decay into neutralinos, which in turn decay into a gravitino, at least one photon, and jets. No significant deviations from the predictions of the Standard Model are observed. Upper limits are set on the visible cross section due to physics beyond the Standard Model, and lower limits are set on the masses of the gluinos and neutralinos, all at 95% confidence level. Visible cross sections greater than 0.022 fb are excluded and pair-produced gluinos with masses up to 2200 GeV are excluded for most of the NLSP masses investigated.
This paper presents direct searches for lepton flavour violation in Higgs boson decays, $H\rightarrow e\tau$ and $H\rightarrow\mu\tau$, performed using data collected with the ATLAS detector at the LHC. The searches are based on a data sample of proton-proton collisions at a centre-of-mass energy $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of 138 fb$^{-1}$. Leptonic ($\tau \rightarrow \ell \nu_\ell \nu_\tau$) and hadronic ($\tau \rightarrow $ hadrons $ \nu_\tau$) decays of the $\tau$-lepton are considered. Two background estimation techniques are employed: the MC-template method, based on data-corrected simulation samples, and the Symmetry method, based on exploiting the symmetry between electrons and muons in the Standard Model backgrounds. No significant excess of events is observed and the results are interpreted as upper limits on lepton-flavour-violating branching ratios of the Higgs boson. The observed (expected) upper limits set on the branching ratios at 95% confidence level, $\mathcal{B}(H\rightarrow e\tau)<0.20\%$ (0.12%) and $\mathcal{B}(H\rightarrow \mu\tau)<0.18\%$ (0.09%), are obtained with the MC-template method from a simultaneous measurement of potential $H \rightarrow e\tau$ and $H \rightarrow\mu\tau$ signals. The best-fit branching ratio difference, $\mathcal{B}(H\rightarrow \mu\tau)- \mathcal{B}(H\rightarrow e\tau)$, measured with the Symmetry method in the channel where the $\tau$-lepton decays to leptons, is (0.25 $\pm$ 0.10)%, compatible with a value of zero within 2.5$\sigma$.
Fit results of the independent searches (1 POI) showing upper limits at 95% C.L. on the LFV branching ratios of the Higgs boson $H\to e\tau$. The results from standalone channel/categories fits are compared with the results of the combined fit.
Fit results of the independent searches (1 POI) showing upper limits at 95% C.L. on the LFV branching ratios of the Higgs boson $H\to e\tau$. The results from standalone channel/categories fits are compared with the results of the combined fit.
NN score distribution, after an independent fit of the $H\to \mu\tau$ signal, obtained by fitting the data of the Symmetry $\ell\tau_{\ell'}$ channel, for the $\mu\tau_{e}$ final state in the non-VBF category.
A measurement of prompt photon-pair production in proton-proton collisions at $\sqrt{s}=13$ TeV is presented. The data were recorded by the ATLAS detector at the LHC with an integrated luminosity of 139 fb$^{-1}$. Events with two photons in the well-instrumented region of the detector are selected. The photons are required to be isolated and have a transverse momentum of $p_\mathrm{T,\gamma_{1(2)}} > 40(30)$ GeV for the leading (sub-leading) photon. The differential cross sections as functions of several observables for the diphoton system are measured and compared with theoretical predictions from state-of-the-art Monte Carlo and fixed-order calculations. The QCD predictions from next-to-next-to-leading-order calculations and multi-leg merged calculations are able to describe the measured integrated and differential cross sections within uncertainties, whereas lower-order calculations show significant deviations, demonstrating that higher-order perturbative QCD corrections are crucial for this process. The resummed predictions with parton showers additionally provide an excellent description of the low transverse-momentum regime of the diphoton system.
This paper reports a measurement of the cross section for the pair production of top quarks in ppbar collisions at sqrt(s) = 1.96 TeV at the Fermilab Tevatron. The data was collected from the CDF II detector in a set of runs with a total integrated luminosity of 1.1 fb^{-1}. The cross section is measured in the dilepton channel, the subset of ttbar events in which both top quarks decay through t -> Wb -> l nu b where l = e, mu, or tau. The lepton pair is reconstructed as one identified electron or muon and one isolated track. The use of an isolated track to identify the second lepton increases the ttbar acceptance, particularly for the case in which one W decays as W -> tau nu. The purity of the sample may be further improved at the cost of a reduction in the number of signal events, by requiring an identified b-jet. We present the results of measurements performed with and without the request of an identified b-jet. The former is the first published CDF result for which a b-jet requirement is added to the dilepton selection. In the CDF data there are 129 pretag lepton + track candidate events, of which 69 are tagged. With the tagging information, the sample is divided into tagged and untagged sub-samples, and a combined cross section is calculated by maximizing a likelihood. The result is sigma_{ttbar} = 9.6 +/- 1.2 (stat.) -0.5 +0.6 (sys.) +/- 0.6 (lum.) pb, assuming a branching ratio of BR(W -> ell nu) = 10.8% and a top mass of m_t = 175 GeV/c^2.
The process e+e- --> pi+ pi- pi0 gamma has been studied at a center-of-mass energy near the Y(4S) resonance using a 89.3 fb-1 data sample collected with the BaBar detector at the PEP-II collider. From the measured 3pi mass spectrum we have obtained the products of branching fractions for the omega and phi mesons, B(omega --> e+e-)B(omega --> 3pi)=(6.70 +/- 0.06 +/- 0.27)10-5 and B(phi --> e+e-)B(phi --> 3pi)=(4.30 +/- 0.08 +/- 0.21)10-5, and evaluated the e+e- --> pi+ pi- pi0 cross section for the e+e- center-of-mass energy range 1.05 to 3.00 GeV. About 900 e+e- --> J/psi gamma --> pi+ pi- pi0 gamma events have been selected and the branching fraction B(J/psi --> pi+ pi- pi0)=(2.18 +/- 0.19)% has been measured.
We have studied high-energy proton scattering on Be, C, Cu and Pb targets using a single-arm spectrometer. The projectile momenta were 19 and 24 GeV/ c , the square of the four-momentum transfer varied from t = 0.1 to t = 4.4 GeV 2 . We have recorded momentum distributions of scattered protons in the high-momentum range. An application of multiple-scattering theory yielded agreement of calculation and experimental results to within a ± 30% uncertainty of the former.
Measurements of neutral pion production at midrapidity in sqrt(s_NN) = 200 GeV Au+Au collisions as a function of transverse momentum, p_T, collision centrality, and angle with respect to reaction plane are presented. The data represent the final pi^0 results from the PHENIX experiment for the first RHIC Au+Au run at design center-of-mass-energy. They include additional data obtained using the PHENIX Level-2 trigger with more than a factor of three increase in statistics over previously published results for p_T > 6 GeV/c. We evaluate the suppression in the yield of high-p_T pi^0's relative to point-like scaling expectations using the nuclear modification factor R_AA. We present the p_T dependence of R_AA for nine bins in collision centrality. We separately integrate R_AA over larger p_T bins to show more precisely the centrality dependence of the high-p_T suppression. We then evaluate the dependence of the high-p_T suppression on the emission angle \Delta\phi of the pions with respect to event reaction plane for 7 bins in collision centrality. We show that the yields of high-p_T pi^0's vary strongly with \Delta\phi, consistent with prior measurements. We show that this variation persists in the most peripheral bin accessible in this analysis. For the peripheral bins we observe no suppression for neutral pions produced aligned with the reaction plane while the yield of pi^0's produced perpendicular to the reaction plane is suppressed by more than a factor of 2. We analyze the combined centrality and \Delta\phi dependence of the pi^0 suppression in different p_T bins using different possible descriptions of parton energy loss dependence on jet path-length averages to determine whether a single geometric picture can explain the observed suppression pattern.
We report measurement of the cross section of $e^+e^-\to \pi^+\pi^-\psi(2S)$ between 4.0 and $5.5 {\rm GeV}$, based on an analysis of initial state radiation events in a $980 \rm fb^{-1}$ data sample recorded with the Belle detector. The properties of the $Y(4360)$ and $Y(4660)$ states are determined. Fitting the mass spectrum of $\pi^+\pi^-\psi(2S)$ with two coherent Breit-Wigner functions, we find two solutions with identical mass and width but different couplings to electron-positron pairs: $M_{Y(4360)} = (4347\pm 6\pm 3) {\rm MeV}/c^2$, $\Gamma_{Y(4360)} = (103\pm 9\pm 5) {\rm MeV}$, $M_{Y(4660)} = (4652\pm10\pm 8) {\rm MeV}/c^2$, $\Gamma_{Y(4660)} = (68\pm 11\pm 1) \rm MeV$; and ${\cal{B}}[Y(4360)\to \pi^+\pi^-\psi(2S)]\cdot \Gamma_{Y(4360)}^{e^+e^-} = (10.9\pm 0.6\pm 0.7) \rm eV$ and ${\cal{B}}[Y(4660)\to \pi^+\pi^-\psi(2S)]\cdot \Gamma_{Y(4660)}^{e^+e^-} = (8.1\pm 1.1\pm 0.5) \rm eV$ for one solution; or ${\cal{B}}[Y(4360)\to \pi^+\pi^-\psi(2S)]\cdot \Gamma_{Y(4360)}^{e^+e^-} = (9.2\pm 0.6\pm 0.6) \rm eV$ and ${\cal{B}}[Y(4660)\to \pi^+\pi^-\psi(2S)]\cdot \Gamma_{Y(4660)}^{e^+e^-} = (2.0\pm 0.3\pm 0.2) \rm eV$ for the other. Here, the first errors are statistical and the second systematic. Evidence for a charged charmoniumlike structure at $4.05 {\rm GeV}/c^2$ is observed in the $\pi^{\pm}\psi(2S)$ intermediate state in the $Y(4360)$ decays.
None
Average charged multiplicities have been measured separately in $b$, $c$ and light quark ($u,d,s$) events from $Z~0$ decays measured in the SLD experiment. Impact parameters of charged tracks were used to select enriched samples of $b$ and light quark events, and reconstructed charmed mesons were used to select $c$ quark events. We measured the charged multiplicities: $\bar{n}_{uds} = 20.21 \pm 0.10 (\rm{stat.})\pm 0.22(\rm{syst.})$, $\bar{n}_{c} = 21.28 \pm 0.46(\rm{stat.}) ~{+0.41}_{-0.36}(\rm{syst.})$ $\bar{n}_{b} = 23.14 \pm 0.10(\rm{stat.}) ~{+0.38}_{-0.37}(\rm{syst.})$, from which we derived the differences between the total average charged multiplicities of $c$ or $b$ quark events and light quark events: $\Delta \bar{n}_c = 1.07 \pm 0.47(\rm{stat.})~{+0.36}_{-0.30}(\rm{syst.})$ and $\Delta \bar{n}_b = 2.93 \pm 0.14(\rm{stat.})~{+0.30}_{-0.29}(\rm{syst.})$. We compared these measurements with those at lower center-of-mass energies and with perturbative QCD predictions. These combined results are in agreement with the QCD expectations and disfavor the hypothesis of flavor-independent fragmentation.
Using data collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider, we measure the energy dependence of the $e^+e^- \to h_b(nP)\pi^+\pi^-$ $(n=1,2)$ cross sections from thresholds up to $11.02\,$GeV. We find clear $\Upsilon(10860)$ and $\Upsilon(11020)$ peaks with little or no continuum contribution. We study the resonant substructure of the $\Upsilon(11020) \to h_b(nP)\pi^+\pi^-$ transitions and find evidence that they proceed entirely via the intermediate isovector states $Z_b(10610)$ and $Z_b(10650)$. The relative fraction of these states is loosely constrained by the current data: the hypothesis that only $Z_b(10610)$ is produced is excluded at the level of 3.3 standard deviations, while the hypothesis that only $Z_b(10650)$ is produced is not excluded at a significant level.
The differential cross section for the reaction e + e − → γγ has been measured in the CMS energy range between 9.4 and 31.6 GeV. The results are found to be in agreement with the predictions of quantum electrodynamics up to momentum transfers- q 2 of 900 GeV 2 . The data set lower limits of about 40 GeV on QED cut-off parameters. We have searched for the decay υ (9.46) → γγ and obtain an upper limit Γ ( υ → γγ )/ Γ ( υ → all) < 1.4% (95% c.l.).
We present a measurement of the top quark mass and of the top-antitop pair production cross section using p-pbar data collected with the CDFII detector at the Tevatron Collider at the Fermi National Accelerator Laboratory and corresponding to an integrated luminosity of 2.9 fb-1. We select events with six or more jets satisfying a number of kinematical requirements imposed by means of a neural network algorithm. At least one of these jets must originate from a b quark, as identified by the reconstruction of a secondary vertex inside the jet. The mass measurement is based on a likelihood fit incorporating reconstructed mass distributions representative of signal and background, where the absolute jet energy scale (JES) is measured simultaneously with the top quark mass. The measurement yields a value of 174.8 +- 2.4(stat+JES) ^{+1.2}_{-1.0}(syst) GeV/c^2, where the uncertainty from the absolute jet energy scale is evaluated together with the statistical uncertainty. The procedure measures also the amount of signal from which we derive a cross section, sigma_{ttbar} = 7.2 +- 0.5(stat) +- 1.0 (syst) +- 0.4 (lum) pb, for the measured values of top quark mass and JES.
The cross section for e+e- to pi+ pi- psi(2S) between threshold and \sqrt{s}=5.5 GeV is measured using 673 fb^{-1} of data on and off the \Upsilon(4S) resonance collected with the Belle detector at KEKB. Two resonant structures are observed in the pi+ pi- psi(2S) invariant mass distribution, one at 4361\pm 9\pm 9 MeV/c2 with a width of 74\pm 15\pm 10 MeV/c2, and another at 4664\pm 11\pm 5 MeV/c2 with a width of 48\pm 15\pm 3 MeV/c2, if the mass spectrum is parameterized with the coherent sum of two Breit-Wigner functions. These values do not match those of any of the known charmonium states.
A generic search for resonances is performed with events containing a $Z$ boson with transverse momentum greater than 100 GeV, decaying into $e^+e^-$ or $\mu^+\mu^-$. The analysed data collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider correspond to an integrated luminosity of 139 fb$^{-1}$. Two invariant mass distributions are examined for a localised excess relative to the expected Standard Model background in six independent event categories (and their inclusive sum) to increase the sensitivity. No significant excess is observed. Exclusion limits at 95% confidence level are derived for two cases: a model-independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass, and a specific heavy vector triplet model with the decay mode $W'\to ZW \to \ell\ell qq$.
A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved'' channel) and topologies with boosted final states with hadronic and/or leptonic products partially overlapping and reconstructed as a large-radius jet (``boosted'' channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})<1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos. These constitute the most stringent exclusion limits to date for the model considered.
The $m_{eejj}$ distribution in the resolved electron channel.
The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of phi meson production in the K+K- decay channel at midrapidity in p+p, d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV. Results are presented on the phi invariant yield and the nuclear modification factor R_AA for Au+Au and Cu+Cu, and R_dA for d+Au collisions, studied as a function of transverse momentum (1<p_T<7 GeV/c) and centrality. In central and mid-central Au+Au collisions, the R_AA of phi exhibits a suppression relative to expectations from binary scaled p+p results. The amount of suppression is smaller than that of the neutral pion and the eta meson in the intermediate p_T range (2--5 GeV/c); whereas at higher p_T the phi, pi^0, and eta show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate p_T is not observed for the phi meson despite the similar mass of the proton and the phi. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the R_AA values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of N_part. The R_dA of phi shows no evidence for cold nuclear effects within uncertainties.
An inclusive search for long-lived exotic particles decaying to a pair of muons is presented. The search uses data collected by the CMS experiment at the CERN LHC in proton-proton collisions at $\sqrt{s}$ = 13 TeV in 2016 and 2018 and corresponding to an integrated luminosity of 97.6 fb$^{-1}$. The experimental signature is a pair of oppositely charged muons originating from a common secondary vertex spatially separated from the pp interaction point by distances ranging from several hundred $\mu$m to several meters. The results are interpreted in the frameworks of the hidden Abelian Higgs model, in which the Higgs boson decays to a pair of long-lived dark photons Z$_\mathrm{D}$, and of a simplified model, in which long-lived particles are produced in decays of an exotic heavy neutral scalar boson. For the hidden Abelian Higgs model with $m_\mathrm{Z_D}$ greater than 20 GeV and less than half the mass of the Higgs boson, they provide the best limits to date on the branching fraction of the Higgs boson to dark photons for $c\tau$(Z$_\mathrm{D}$) (varying with $m_\mathrm{Z_D}$) between 0.03 and ${\approx}$ 0.5 mm, and above ${\approx}$ 0.5 m. Our results also yield the best constraints on long-lived particles with masses larger than 10 GeV produced in decays of an exotic scalar boson heavier than the Higgs boson and decaying to a pair of muons.
Differential and total cross sections for the quasifree reactions $\gamma p\rightarrow\eta p$ and $\gamma n\rightarrow\eta n$ have been determined at the MAMI-C electron accelerator using a liquid deuterium target. Photons were produced via bremsstrahlung from the 1.5 GeV incident electron beam and energy-tagged with the Glasgow photon tagger. Decay photons of the neutral decay modes $\eta\rightarrow 2\gamma$ and $\eta\rightarrow 3\pi^0 \rightarrow 6\gamma$ and coincident recoil nucleons were detected in a combined setup of the Crystal Ball and the TAPS calorimeters. The $\eta$-production cross sections were measured in coincidence with recoil protons, recoil neutrons, and in an inclusive mode without a condition on recoil nucleons, which allowed a check of the internal consistency of the data. The effects from nuclear Fermi motion were removed by a kinematic reconstruction of the final-state invariant mass and possible nuclear effects on the quasifree cross section were investigated by a comparison of free and quasifree proton data. The results, which represent a significant improvement in statistical quality compared to previous measurements, agree with the known neutron-to-proton cross-section ratio in the peak of the $S_{11}(1535)$ resonance and confirm a peak in the neutron cross section, which is absent for the proton, at a center-of-mass energy $W = (1670\pm 5)$ MeV with an intrinsic width of $\Gamma\approx 30$ MeV.
The transversity distribution, which describes transversely polarized quarks in transversely polarized nucleons, is a fundamental component of the spin structure of the nucleon, and is only loosely constrained by global fits to existing semi-inclusive deep inelastic scattering (SIDIS) data. In transversely polarized $p^\uparrow+p$ collisions it can be accessed using transverse polarization dependent fragmentation functions which give rise to azimuthal correlations between the polarization of the struck parton and the final state scalar mesons. This letter reports on spin dependent di-hadron correlations measured by the STAR experiment. The new dataset corresponds to 25 pb$^{-1}$ integrated luminosity of $p^\uparrow+p$ collisions at $\sqrt{s}=500$ GeV, an increase of more than a factor of ten compared to our previous measurement at $\sqrt{s}=200$ GeV. Non-zero asymmetries sensitive to transversity are observed at a $Q^2$ of several hundred GeV and are found to be consistent with the former measurement and a model calculation. %we observe consistent with the former measurement are observed.} We expect that these data will enable an extraction of transversity with comparable precision to current SIDIS datasets but at much higher momentum transfers where subleading effects are suppressed.
Charged hadrons in 0.15 < pt < 4 GeV/c associated with particles of pt^trig > 4 GeV/c are reconstructed in pp and Au+Au collisions at sqrt(s_NN)=200 GeV. The associated multiplicity and pt magnitude sum are found to increase from pp to central Au+Au collisions. The associated pt distributions, while similar in shape on the near side, are significantly softened on the away side in central Au+Au relative to pp and not much harder than that of inclusive hadrons. The results, consistent with jet quenching, suggest that the away-side fragments approach equilibration with the medium traversed.
We have measured the polarization of J/Psi and Psi(2S) mesons produced in p\bar{p} collisions at \sqrt{s} = 1.8 TeV, using data collected at CDF during 1992-95. The polarization of promptly produced J/Psi [Psi(2S)] mesons is isolated from those produced in B-hadron decay, and measured over the kinematic range 4[5.5] < P_T < 20 GeV/c and |y| < 0.6. For P_T \gessim 12 GeV/c we do not observe significant polarization in the prompt component.
A measurement of inclusive and differential fiducial cross-sections for the production of the Higgs boson decaying into two photons is performed using $139~\text{fb}^{-1}$ 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, in a fiducial region closely matching the experimental selection, is measured to be $67\pm 6$ fb, which is in agreement with the state-of-the-art Standard Model prediction of $64\pm 4$ fb. Extrapolating this result to the full phase space and correcting for the branching ratio, the total cross-section for Higgs boson production is estimated to be $58\pm 6$ pb. In addition, the cross-sections in four fiducial regions sensitive to various Higgs boson production modes and differential cross-sections as a function of either one or two of several observables are measured. All the measurements are found to be in agreement with the Standard Model predictions. The measured transverse momentum distribution of the Higgs boson is used as an indirect probe of the Yukawa coupling of the Higgs boson to the bottom and charm quarks. In addition, five differential cross-section measurements are used to constrain anomalous Higgs boson couplings to vector bosons in the Standard Model effective field theory framework.
High-energy nuclear collisions create an energy density similar to that of the universe microseconds after the Big Bang, and in both cases, matter and antimatter are formed with comparable abundance. However, the relatively short-lived expansion in nuclear collisions allows antimatter to decouple quickly from matter, and avoid annihilation. Thus, a high energy accelerator of heavy nuclei is an efficient means of producing and studying antimatter. The antimatter helium-4 nucleus ($^4\bar{He}$), also known as the anti-{\alpha} ($\bar{\alpha}$), consists of two antiprotons and two antineutrons (baryon number B=-4). It has not been observed previously, although the {\alpha} particle was identified a century ago by Rutherford and is present in cosmic radiation at the 10% level. Antimatter nuclei with B < -1 have been observed only as rare products of interactions at particle accelerators, where the rate of antinucleus production in high-energy collisions decreases by about 1000 with each additional antinucleon. We present the observation of the antimatter helium-4 nucleus, the heaviest observed antinucleus. In total 18 $^4\bar{He}$ counts were detected at the STAR experiment at RHIC in 10$^9$ recorded Au+Au collisions at center-of-mass energies of 200 GeV and 62 GeV per nucleon-nucleon pair. The yield is consistent with expectations from thermodynamic and coalescent nucleosynthesis models, which has implications beyond nuclear physics.
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/>
$|{y}^{t,1}|\otimes |{y}^{t,2}|$ absolute differential cross-section at particle level, for 0.2 < $|{y}^{t,1}|$ < 0.5.
We have used 87 pb^-1 of data collected with the Collider Detector at Fermilab to search for new particles decaying to b bbar. We present model-independent upper limits on the cross section for narrow resonances which excludes the color-octet technirho in the mass interval 350 < M < 440 GeV/c^2. In addition, we exclude topgluons, predicted in models of topcolor-assisted technicolor, of width Gamma = 0.3 M in the mass range 280 < M < 670 GeV/c^2, of width Gamma = 0.5 M in the mass range 340 < M < 640 GeV/c^2, and of width Gamma = 0.7 M in the mass range 375 < M < 560 GeV/c^2.
We report on a study of the transverse momentum dependence of nuclear modification factors $R_{dAu}$ for charged hadrons produced in deuteron + gold collisions at $\sqrt{s_{NN}=\unit[200]{GeV}$, as a function of collision centrality and of the pseudorapidity ($\eta = 0,1,2.2,3.2 $) of the produced hadrons. We find significant and systematic decrease of $R_{dAu}$ with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at RHIC energies.
Forum