This Letter reports a measurement of the cross section for producing pairs of central prompt isolated photons in proton-antiproton collisions at a total energy of 1.96 TeV using data corresponding to 9.5/fb integrated luminosity collected with the CDF II detector at the Fermilab Tevatron. The measured differential cross section is compared to three calculations derived from the theory of strong interactions. These include a prediction based on a leading order matrix element calculation merged with parton shower, a next-to-leading order, and a next-to-next-to-leading order calculation. The first and last calculations reproduce most aspects of the data, thus showing the importance of higher-order contributions for understanding the theory of strong interaction and improving measurements of the Higgs boson and searches for new phenomena in diphoton final states.
The measured differential cross sections for the photon $E_T$ (two entries per event) , together with the predictions from the Sherpa Monte Carlo.
Two-particle azimuthal ($\Delta\phi$) and pseudorapidity ($\Delta\eta$) correlations using a trigger particle with large transverse momentum ($p_T$) in $d$+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{{NN}}}$ =\xspace 62.4 GeV and 200~GeV from the STAR experiment at RHIC are presented. The \ns correlation is separated into a jet-like component, narrow in both $\Delta\phi$ and $\Delta\eta$, and the ridge, narrow in $\Delta\phi$ but broad in $\Delta\eta$. Both components are studied as a function of collision centrality, and the jet-like correlation is studied as a function of the trigger and associated $p_T$. The behavior of the jet-like component is remarkably consistent for different collision systems, suggesting it is produced by fragmentation. The width of the jet-like correlation is found to increase with the system size. The ridge, previously observed in Au+Au collisions at $\sqrt{s_{{NN}}}$ = 200 GeV, is also found in Cu+Cu collisions and in collisions at $\sqrt{s_{{NN}}}$ =\xspace 62.4 GeV, but is found to be substantially smaller at $\sqrt{s_{{NN}}}$ =\xspace 62.4 GeV than at $\sqrt{s_{{NN}}}$ = 200 GeV for the same average number of participants ($ \langle N_{\mathrm{part}}\rangle$). Measurements of the ridge are compared to models.
Dependence of the widths in $\Delta\eta$ on $p_T^{\mathrm{associated}}$ for 3 $<$ $p_T^{trigger}$ $<$ 6 GeV/$c$ for 0-95% $d$+Au, 0-60% Cu+Cu at $\sqrt{s_{NN}}$ = 62.4 GeV and $\sqrt{s_{NN}}$ = 200 GeV, 0-80% Au+Au at $\sqrt{s_{NN}}$ = 62.4 GeV, and 0-12% and 40-80% Au+Au at $\sqrt{s_{NN}}$ = 200 GeV.
We present the first measurements of identified hadron production, azimuthal anisotropy, and pion interferometry from Au+Au collisions below the nominal injection energy at the Relativistic Heavy-Ion Collider (RHIC) facility. The data were collected using the large acceptance STAR detector at $\sqrt{s_{NN}}$ = 9.2 GeV from a test run of the collider in the year 2008. Midrapidity results on multiplicity density (dN/dy) in rapidity (y), average transverse momentum (<pT>), particle ratios, elliptic flow, and HBT radii are consistent with the corresponding results at similar $\sqrt{s_{NN}}$ from fixed target experiments. Directed flow measurements are presented for both midrapidity and forward rapidity regions. Furthermore the collision centrality dependence of identified particle dN/dy, <pT>, and particle ratios are discussed. These results also demonstrate the readiness of the STAR detector to undertake the proposed QCD critical point search and the exploration of the QCD phase diagram at RHIC.
v1 as a function of eta and eta/y-beam from different experiments and methods.
Balance functions have been measured for charged particle pairs, identified charged pion pairs, and identified charged kaon pairs in Au+Au, d+Au, and p+p collisions at $\sqrt{s_{NN}}$ = 200 GeV at the Relativistic Heavy Ion Collider using the STAR detector. These balance functions are presented in terms of relative pseudorapidity, $\Delta \eta$, relative rapidity, $\Delta y$, relative azimuthal angle, $\Delta \phi$, and invariant relative momentum, $q_{\rm inv}$. In addition, balance functions are shown in terms of the three components of $q_{\rm inv}$: $q_{\rm long}$, $q_{\rm out}$, and $q_{\rm side}$. For charged particle pairs, the width of the balance function in terms of $\Delta \eta$ scales smoothly with the number of participating nucleons, while HIJING and UrQMD model calculations show no dependence on centrality or system size. For charged particle and charged pion pairs, the balance functions widths in terms of $\Delta \eta$ and $\Delta y$ are narrower in central Au+Au collisions than in peripheral collisions. The width for central collisions is consistent with thermal blast-wave models where the balancing charges are highly correlated in coordinate space at breakup. This strong correlation might be explained either by delayed hadronization or by limited diffusion during the reaction. Furthermore, the narrowing trend is consistent with the lower kinetic temperatures inherent to more central collisions. In contrast, the width of the balance function for charged kaon pairs in terms of $\Delta y$ shows little centrality dependence, which may signal a different production mechanism for kaons. The widths of the balance functions for charged pions and kaons in terms of $q_{\rm inv}$ narrow in central collisions compared to peripheral collisions, which may be driven by the change in the kinetic temperature.
(Color online) The widths for the balance functions for pions in terms of $q_{long}$, $q_{out}$, and $q_{side}$ compared with UrQMD calculations.
Elliptic flow ($v_{2}$) values for identified particles at mid-rapidity in Au+Au collisions, measured by the STAR experiment in the Beam Energy Scan at RHIC at $\sqrt{s_{NN}}=$ 7.7--62.4 GeV, are presented. A beam-energy dependent difference of the values of $v_{2}$ between particles and corresponding anti-particles was observed. The difference increases with decreasing beam energy and is larger for baryons compared to mesons. This implies that, at lower energies, particles and anti-particles are not consistent with the universal number-of-constituent-quark (NCQ) scaling of $v_{2}$ that was observed at $\sqrt{s_{NN}}=$ 200 GeV.
The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles, frames a) and b), and anti-particles, frames c) and d), in 0-80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4 GeV. Simultaneous fits to the mesons except the pions are shown as the dashed lines. The difference of the baryon $v_{2}$ and the meson fits are shown in the lower panels.
Dihadron azimuthal correlations containing a high transverse momentum ($p_T$) trigger particle are sensitive to the properties of the nuclear medium created at RHIC through the strong interactions occurring between the traversing parton and the medium, i.e. jet-quenching. Previous measurements revealed a strong modification to dihadron azimuthal correlations in Au+Au collisions with respect to p+p and d+Au collisions. The modification increases with the collision centrality, suggesting a path-length or energy density dependence to the jet-quenching effect. This paper reports STAR measurements of dihadron azimuthal correlations in mid-central (20-60%) Au+Au collisions at $\sqrt{s_{_{\rm NN}}}=200$ GeV as a function of the trigger particle's azimuthal angle relative to the event plane, $\phi_s=|\phi_t-\psi_{\rm EP}|$. The azimuthal correlation is studied as a function of both the trigger and associated particle $p_T$. The subtractions of the combinatorial background and anisotropic flow, assuming Zero Yield At Minimum (ZYAM), are described. The correlation results are first discussed with subtraction of the even harmonic (elliptic and quadrangular) flow backgrounds. The away-side correlation is strongly modified, and the modification varies with $\phi_s$, with a double-peak structure for out-of-plane trigger particles. The near-side ridge (long range pseudo-rapidity $\Delta\eta$ correlation) appears to drop with increasing $\phi_s$ while the jet-like component remains approximately constant. The correlation functions are further studied with subtraction of odd harmonic triangular flow background arising from fluctuations. It is found that the triangular flow, while responsible for the majority of the amplitudes, is not sufficient to explain the $\phi_s$-dependence of the ridge or the away-side double-peak structure. ...
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
We present results on strange and multi-strange particle production in Au+Au collisions at $\sqrt{s_{NN}}=62.4$ GeV as measured with the STAR detector at RHIC. Mid-rapidity transverse momentum spectra and integrated yields of $K^{0}_{S}$, $\Lambda$, $\Xi$, $\Omega$ and their anti-particles are presented for different centrality classes. The particle yields and ratios follow a smooth energy dependence. Chemical freeze-out parameters, temperature, baryon chemical potential and strangeness saturation factor obtained from the particle yields are presented. Intermediate transverse momentum ($p_T$) phenomena are discussed based on the ratio of the measured baryon-to-meson spectra and nuclear modification factor. The centrality dependence of various measurements presented show a similar behavior as seen in Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV.
Temperature and baryon chemical potential obtained from thermal model fits as a function of √sNN (see Ref. [22]). The dashed lines correspond to the parametrizations given in Ref. [22]. The solid stars show the result for √sNN=62.4 and 200 GeV.
Temperature and baryon chemical potential obtained from thermal model fits as a function of √sNN (see Ref. [22]). The dashed lines correspond to the parametrizations given in Ref. [22]. The solid stars show the result for √sNN=62.4 and 200 GeV.
Temperature and baryon chemical potential obtained from thermal model fits as a function of √sNN (see Ref. [22]). The dashed lines correspond to the parametrizations given in Ref. [22]. The solid stars show the result for √sNN=62.4 and 200 GeV.
We report on K*0 production at mid-rapidity in Au+Au and Cu+Cu collisions at \sqrt{s_{NN}} = 62.4 and 200 GeV collected by the Solenoid Tracker at RHIC (STAR) detector. The K*0 is reconstructed via the hadronic decays K*0 \to K+ pi- and \bar{K*0} \to K-pi+. Transverse momentum, pT, spectra are measured over a range of pT extending from 0.2 GeV/c to 5 GeV/c. The center of mass energy and system size dependence of the rapidity density, dN/dy, and the average transverse momentum, <pT>, are presented. The measured N(K*0)/N(K) and N(\phi)/N(K*0) ratios favor the dominance of re-scattering of decay daughters of K*0 over the hadronic regeneration for the K*0 production. In the intermediate pT region (2.0 < pT < 4.0 GeV/c), the elliptic flow parameter, v2, and the nuclear modification factor, RCP, agree with the expectations from the quark coalescence model of particle production.
Mid-rapidity $K^{*0}$ $p_T$ spectra for various collision centrality bins (0-20%, 20-40%, 40-60%, 60-80%) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
Measurements of the elliptic flow, $v_{2}$, of identified hadrons ($\pi^{\pm}$, $K^{\pm}$, $K_{s}^{0}$, $p$, $\bar{p}$, $\phi$, $\Lambda$, $\bar{\Lambda}$, $\Xi^{-}$, $\bar{\Xi}^{+}$, $\Omega^{-}$, $\bar{\Omega}^{+}$) in Au+Au collisions at $\sqrt{s_{NN}}=$ 7.7, 11.5, 19.6, 27, 39 and 62.4 GeV are presented. The measurements were done at mid-rapidity using the Time Projection Chamber and the Time-of-Flight detectors of the STAR experiment during the Beam Energy Scan program at RHIC. A significant difference in the $v_{2}$ values for particles and the corresponding anti-particles was observed at all transverse momenta for the first time. The difference increases with decreasing center-of-mass energy, $\sqrt{s_{NN}}$ (or increasing baryon chemical potential, $\mu_{B}$) and is larger for the baryons as compared to the mesons. This implies that particles and anti-particles are no longer consistent with the universal number-of-constituent quark (NCQ) scaling of $v_{2}$ that was observed at $\sqrt{s_{NN}}=$ 200 GeV. However, for the group of particles NCQ scaling at $(m_{T}-m_{0})/n_{q}>$ 0.4 GeV/$c^{2}$ is not violated within $\pm$10%. The $v_{2}$ values for $\phi$ mesons at 7.7 and 11.5 GeV are approximately two standard deviations from the trend defined by the other hadrons at the highest measured $p_{T}$ values.
The elliptic flow,v_2, as a function of the transverse momentum,p_T, from 0–80% central Au+Au collisions for various particle species and energies.
A study is reported of the same- and opposite-sign charge-dependent azimuthal correlations with respect to the event plane in Au+Au collisions at 200 GeV. The charge multiplicity asymmetries between the up/down and left/right hemispheres relative to the event plane are utilized. The contributions from statistical fluctuations and detector effects were subtracted from the (co-)variance of the observed charge multiplicity asymmetries. In the mid- to most-central collisions, the same- (opposite-) sign pairs are preferentially emitted in back-to-back (aligned on the same-side) directions. The charge separation across the event plane, measured by the difference, $\Delta$, between the like- and unlike-sign up/down $-$ left/right correlations, is largest near the event plane. The difference is found to be proportional to the event-by-event final-state particle ellipticity (via the observed second-order harmonic $v^{\rm obs}_{2}$), where $\Delta=(1.3\pm1.4({\rm stat})^{+4.0}_{-1.0}({\rm syst}))\times10^{-5}+(3.2\pm0.2({\rm stat})^{+0.4}_{-0.3}({\rm syst}))\times10^{-3}v^{\rm obs}_{2}$ for 20-40% Au+Au collisions. The implications for the proposed chiral magnetic effect are discussed.
The relative charge asymmetry correlations, $\langle A_{+}A_{-}\rangle_{ UD}/\langle A_{+}A_{-}\rangle_{ LR}$, as a function of the number of participants, $N_{part}$, for four combinations of $\eta$ ranges used for EP reconstruction and asymmetry calculation.
Searches for new phenomena inspired by supersymmetry in final states containing an $e^+e^-$ or $\mu^+\mu^-$ pair, jets, and missing transverse momentum are presented. These searches make use of proton-proton collision data with an integrated luminosity of 139 $\text{fb}^{-1}$, collected during 2015-2018 at a centre-of-mass energy $\sqrt{s}=13 $TeV by the ATLAS detector at the Large Hadron Collider. Two searches target the pair production of charginos and neutralinos. One uses the recursive-jigsaw reconstruction technique to follow up on excesses observed in 36.1 $\text{fb}^{-1}$ of data, and the other uses conventional event variables. The third search targets pair production of coloured supersymmetric particles (squarks or gluinos) decaying through the next-to-lightest neutralino $(\tilde\chi_2^0)$ via a slepton $(\tilde\ell)$ or $Z$ boson into $\ell^+\ell^-\tilde\chi_1^0$, resulting in a kinematic endpoint or peak in the dilepton invariant mass spectrum. The data are found to be consistent with the Standard Model expectations. Results are interpreted using simplified models and exclude masses up to 900 GeV for electroweakinos, 1550 GeV for squarks, and 2250 GeV for gluinos.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>EWK SR distributions:</b> <a href="116034?version=1&table=Figure 11a">SR-High_8-EWK</a>; <a href="116034?version=1&table=Figure 11b">SR-ℓℓ𝑏𝑏-EWK</a>; <a href="116034?version=1&table=Figure 11c">SR-Int-EWK</a>; <a href="116034?version=1&table=Figure 11d">SR-Low-EWK</a>; <a href="116034?version=1&table=Figure 11e">SR-OffShell-EWK</a><br/><br/> <b>Strong SR distributions:</b> <a href="116034?version=1&table=Figure 13a">SRC-STR</a>; <a href="116034?version=1&table=Figure 13b">SRLow-STR</a>; <a href="116034?version=1&table=Figure 13c">SRMed-STR</a>; <a href="116034?version=1&table=Figure 13d">SRHigh-STR</a><br/><br/> <b>RJR SR Yields:</b> <a href="116034?version=1&table=Table 16">SR2l-Low-RJR, SR2l-ISR-RJR</a><br/><br/> <b>EWK SR Yields:</b> <a href="116034?version=1&table=Table 18">SR-High_16a-EWK, SR-High_8a-EWK, SR-1J-High-EWK, SR-ℓℓ𝑏𝑏-EWK, SR-High_16b-EWK, SR-High_8b-EWK</a>; <a href="116034?version=1&table=Table 19">SR-Int_a-EWK, SR-Low_a-EWK, SR-Low-2-EWK, SR-OffShell_a-EWK, SR-Int_b-EWK, SR-Low_b-EWK, SR-OffShell_b-EWK </a><br/><br/> <b>Strong SR Yields:</b> <a href="116034?version=1&table=Table 21">SRC-STR, SRLow-STR, SRMed-STR, SRHigh-STR</a>; <a href="116034?version=1&table=Table 22">SRZLow-STR, SRZMed-STR, SRZHigh-STR</a><br/><br/> <b>C1N2 Model Limits:</b> <a href="116034?version=1&table=Table 15a C1N2 Observed Limit">Obs</a>; <a href="116034?version=1&table=Table 15a C1N2 Expected Limit">Exp</a>; <a href="116034?version=1&table=Auxiliary Figure 34a C1N2 Expected XS Upper Limit">Upper Limits</a><br/><br/> <b>GMSB Model Limits:</b> <a href="116034?version=1&table=Table 15b GMSB Observed Limit">Obs</a>; <a href="116034?version=1&table=Table 15b GMSB Expected Limit">Exp</a>; <a href="116034?version=1&table=Auxiliary Figure 34b GMSB Expected XS Upper Limit">Upper Limits</a><br/><br/> <b>Gluon-Slepton Model Limits:</b> <a href="116034?version=1&table=Figure 16a Observed Limit">Obs</a>; <a href="116034?version=1&table=Figure 16a Expected Limit">Exp</a>; <a href="116034?version=1&table=Auxiliary Figure 23a XS Upper Limit">Upper Limits</a><br/><br/> <b>Gluon-Z* Model Limits:</b> <a href="116034?version=1&table=Figure 16b Observed Limit">Obs</a>; <a href="116034?version=1&table=Figure 16b Expected Limit">Exp</a>; <a href="116034?version=1&table=Auxiliary Figure 23b XS Upper Limit">Upper Limits</a><br/><br/> <b>Squark-Z* Model Limits:</b> <a href="116034?version=1&table=Figure 16c Observed Limit">Obs</a>; <a href="116034?version=1&table=Figure 16c Expected Limit">Exp</a>; <a href="116034?version=1&table=Auxiliary Figure 23c XS Upper Limit">Upper Limits</a><br/><br/> <b>EWK VR distributions:</b> <a href="116034?version=1&table=Figure 4a S_ETmiss in VR-High-Sideband-EWK">VR-High-Sideband-EWK</a>; <a href="116034?version=1&table=Figure 4b S_Etmiss in VR-High-R-EWK">VR-High-R-EWK</a>; <a href="116034?version=1&table=Figure 4c S_Etmiss in VR-1J-High-EWK">VR-1J-High-EWK</a>; <a href="116034?version=1&table=Figure 4d S_Etmiss in VR-llbb-EWK">VR-ℓℓ𝑏𝑏-EWK</a>; <a href="116034?version=1&table=Figure 5a S_Etmiss in VR-Int-EWK">VR-Int-EWK</a>; <a href="116034?version=1&table=Figure 5b S_Etmiss in VR-Low-EWK">VR-Low-EWK</a>; <a href="116034?version=1&table=Figure 5c S_Etmiss in VR-Low-2-EWK">VR-Low-2-EWK</a>; <a href="116034?version=1&table=Figure 5d S_Etmiss in VR-OffShell-EWK">VR-OffShell-EWK</a><br/><br/> <b>Strong VR distributions:</b> <a href="116034?version=1&table=Figure 6a">VRC-STR</a>; <a href="116034?version=1&table=Figure 6b">VRLow-STR</a>; <a href="116034?version=1&table=Figure 6c">VRMed-STR</a>; <a href="116034?version=1&table=Figure 6d">VRHigh-STR</a>; <a href="116034?version=1&table=Figure 8">VR3L-STR</a><br/><br/> <b>Other Strong distributions:</b> <a href="116034?version=1&table=Auxiliary Figure 17a">SRLow-STR + VRLow-STR</a><br/><br/> <b>Other EWK distributions:</b> <a href="116034?version=1&table=Auxiliary Figure 33a Mjj in CR-Z-EWK and SR-Low-EWK">CR-Z-EWK + SR-Low-EWK</a>; <a href="116034?version=1&table=Auxiliary Figure 33b S_ETmiss in CR-Z-met-EWK">CR-Z-met-EWK</a><br/><br/> <b>Strong Signal Cutflows:</b> <a href="116034?version=1&table=Auxiliary Table 30-31 SRC-STR Cutflow">SRC-STR GG_N2_ZN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRMed-STR Cutflow">SRC-STR SS_N2_ZN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRLow-STR Cutflow">SRLow-STR GG_N2_SLN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRHigh-STR Cutflow">SRC-STR GG_N2_SLN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRZLow-STR Cutflow">SRZLow-STR SS_N2_ZN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRZMed-STR Cutflow">SRZMed-STR SS_N2_ZN1</a>; <a href="116034?version=1&table=Auxiliary Table 30-31 SRZHigh-STR Cutflow">SRZHigh-STR SS_N2_ZN1</a><br/><br/> <b>EWK Signal Cutflows:</b> <a href="116034?version=1&table=Auxiliary Table 36 SR-OffShell_a-EWK Cutflow"> SR-OffShell_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 37 SR-OffShell_b-EWK Cutflow"> SR-OffShell_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 38 SR-Low_a-EWK Cutflow"> SR-Low_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 39 SR-Low_b-EWK Cutflow"> SR-Low_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 40 SR-Low-2-EWK Cutflow"> SR-Low-2-E</a>; <a href="116034?version=1&table=Auxiliary Table 41 SR-Int_a-EWK Cutflow"> SR-Int_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 42 SR-Int_b-EWK Cutflow"> SR-Int_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 43 SR-High_16a-EWK Cutflow"> SR-High_16a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 44 SR-High_16b-EWK Cutflow"> SR-High_16b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 45 SR-High_8a-EWK Cutflow"> SR-High_8a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 46 SR-High_8b-EWK Cutflow"> SR-High_8b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 47 SR-1J-High-EWK Cutflow"> SR-1J-Hig</a>; <a href="116034?version=1&table=Auxiliary Table 48 SR-llbb-EWK Cutflow"> SR-llbb-EWK</a><br/><br/> <b>EWK Signal Number of MC Events:</b> <a href="116034?version=1&table=Auxiliary Table 36 SR-OffShell_a-EWK Generated"> SR-OffShell_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 37 SR-OffShell_b-EWK Generated"> SR-OffShell_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 38 SR-Low_a-EWK Generated"> SR-Low_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 39 SR-Low_b-EWK Generated"> SR-Low_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 40 SR-Low-2-EWK Generated"> SR-Low-2-E</a>; <a href="116034?version=1&table=Auxiliary Table 41 SR-Int_a-EWK Generated"> SR-Int_a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 42 SR-Int_b-EWK Generated"> SR-Int_b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 43 SR-High_16a-EWK Generated"> SR-High_16a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 44 SR-High_16b-EWK Generated"> SR-High_16b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 45 SR-High_8a-EWK Generated"> SR-High_8a-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 46 SR-High_8b-EWK Generated"> SR-High_8b-EWK</a>; <a href="116034?version=1&table=Auxiliary Table 47 SR-1J-High-EWK Generated"> SR-1J-Hig</a>; <a href="116034?version=1&table=Auxiliary Table 48 SR-llbb-EWK Generated"> SR-llbb-EWK</a><br/><br/> <b>SRC-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_SLN1 acc in SRC">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 acc in SRC">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRC">SS_N2_ZN1</a><br/><br/> <b>SRLow-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_SLN1 acc in SRLow">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 acc in SRLow">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRLow">SS_N2_ZN1</a><br/><br/> <b>SRMed-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_SLN1 acc in SRMed">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 acc in SRMed">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRMed">SS_N2_ZN1</a><br/><br/> <b>SRHigh-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_SLN1 acc in SRHigh">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 acc in SRHigh">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRHigh">SS_N2_ZN1</a><br/><br/> <b>SRZLow-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_ZN1 acc in SRZLow">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRZLow">SS_N2_ZN1</a><br/><br/> <b>SRZMed-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_ZN1 acc in SRZMed">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRZMed">SS_N2_ZN1</a><br/><br/> <b>SRZHigh-STR Signal Acceptance:</b> <a href="116034?version=1&table=GG_N2_ZN1 acc in SRZHigh">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 acc in SRZHigh">SS_N2_ZN1</a><br/><br/> <b>SRC-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_SLN1 eff in SRC">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 eff in SRC">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRC">SS_N2_ZN1</a><br/><br/> <b>SRLow-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_SLN1 eff in SRLow">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 eff in SRLow">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRLow">SS_N2_ZN1</a><br/><br/> <b>SRMed-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_SLN1 eff in SRMed">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 eff in SRMed">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRMed">SS_N2_ZN1</a><br/><br/> <b>SRHigh-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_SLN1 eff in SRHigh">GG_N2_SLN1</a>; <a href="116034?version=1&table=GG_N2_ZN1 eff in SRHigh">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRHigh">SS_N2_ZN1</a><br/><br/> <b>SRZLow-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_ZN1 eff in SRZLow">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRZLow">SS_N2_ZN1</a><br/><br/> <b>SRZMed-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_ZN1 eff in SRZMed">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRZMed">SS_N2_ZN1</a><br/><br/> <b>SRZHigh-STR Signal Efficiency:</b> <a href="116034?version=1&table=GG_N2_ZN1 eff in SRZHigh">GG_N2_ZN1</a>; <a href="116034?version=1&table=SS_N2_ZN1 eff in SRZHigh">SS_N2_ZN1</a><br/><br/> <b>SR-OffShell_a-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-OffShell_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-OffShell_a-EWK">C1N2</a>; <br/><br/> <b>SR-OffShell_b-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-OffShell_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-OffShell_b-EWK">C1N2</a>; <br/><br/> <b>SR-Low_a-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in C1N2 acc in SR-Low_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in C1N2 acc in SR-Low_a-EWK">C1N2</a>; <br/><br/> <b>SR-Low_b-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-Low_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-Low_b-EWK">C1N2</a>; <br/><br/> <b>SR-Int_a-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-Int_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-Int_a-EWK">C1N2</a>; <br/><br/> <b>SR-Int_b-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-Int_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-Int_b-EWK">C1N2</a>; <br/><br/> <b>SR-High_16a-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-High_16a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-High_16a-EWK">C1N2</a>; <br/><br/> <b>SR-High_16b-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-High_16b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-High_16b-EWK">C1N2</a>; <br/><br/> <b>SR-High_8a-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-High_8a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-High_8a-EWK">C1N2</a>; <br/><br/> <b>SR-High_8b-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-High_8b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-High_8b-EWK">C1N2</a>; <br/><br/> <b>SR-1J-High-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-1J-High-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-1J-High-EWK">C1N2</a>; <br/><br/> <b>SR-llbb-EWK Signal Acceptance:</b><a href="116034?version=1&table=GMSB acc in SR-llbb-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 acc in SR-llbb-EWK">C1N2</a>; <br/><br/> <b>SR-OffShell_a-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-OffShell_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-OffShell_a-EWK">C1N2</a>; <br/><br/> <b>SR-OffShell_b-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-OffShell_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-OffShell_b-EWK">C1N2</a>; <br/><br/> <b>SR-Low_a-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in C1N2 eff in SR-Low_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in C1N2 eff in SR-Low_a-EWK">C1N2</a>; <br/><br/> <b>SR-Low_b-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-Low_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-Low_b-EWK">C1N2</a>; <br/><br/> <b>SR-Int_a-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-Int_a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-Int_a-EWK">C1N2</a>; <br/><br/> <b>SR-Int_b-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-Int_b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-Int_b-EWK">C1N2</a>; <br/><br/> <b>SR-High_16a-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-High_16a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-High_16a-EWK">C1N2</a>; <br/><br/> <b>SR-High_16b-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-High_16b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-High_16b-EWK">C1N2</a>; <br/><br/> <b>SR-High_8a-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-High_8a-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-High_8a-EWK">C1N2</a>; <br/><br/> <b>SR-High_8b-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-High_8b-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-High_8b-EWK">C1N2</a>; <br/><br/> <b>SR-1J-High-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-1J-High-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-1J-High-EWK">C1N2</a>; <br/><br/> <b>SR-llbb-EWK Signal Efficiency:</b><a href="116034?version=1&table=GMSB eff in SR-llbb-EWK">GMSB</a>; <a href="116034?version=1&table=C1N2 eff in SR-llbb-EWK">C1N2</a>; <br/><br/> <b>Truth Code snippets</b>, <b>SLHA files</b>, and <b>PYHF json likelihoods</b> are available under "Resources" (purple button on the left) ---- Record created with hepdata_lib 0.7.0: https://zenodo.org/record/4946277 and PYHF: https://doi.org/10.5281/zenodo.1169739
Breakdown of expected and observed yields in the three on-$Z$ signal regions after a separate simultaneous fit to each signal region and control region pair. The uncertainties include both the statistical and systematic sources.
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 report the beam energy (\sqrt s_{NN} = 7.7 - 200 GeV) and collision centrality dependence of the mean (M), standard deviation (\sigma), skewness (S), and kurtosis (\kappa) of the net-proton multiplicity distributions in Au+Au collisions. The measurements are carried out by the STAR experiment at midrapidity (|y| < 0.5) and within the transverse momentum range 0.4 < pT < 0.8 GeV/c in the first phase of the Beam Energy Scan program at the Relativistic Heavy Ion Collider. These measurements are important for understanding the Quantum Chromodynamic (QCD) phase diagram. The products of the moments, S\sigma and \kappa\sigma^{2}, are sensitive to the correlation length of the hot and dense medium created in the collisions and are related to the ratios of baryon number susceptibilities of corresponding orders. The products of moments are found to have values significantly below the Skellam expectation and close to expectations based on independent proton and anti-proton production. The measurements are compared to a transport model calculation to understand the effect of acceptance and baryon number conservation, and also to a hadron resonance gas model.
Collision energy and centrality dependence of the net-proton $S\sigma$ and $\kappa\sigma^2$ from Au+Au and p+p collisions at RHIC.
We report the first measurements of the kurtosis (\kappa), skewness (S) and variance (\sigma^2) of net-proton multiplicity (N_p - N_pbar) distributions at midrapidity for Au+Au collisions at \sqrt(s_NN) = 19.6, 62.4, and 200 GeV corresponding to baryon chemical potentials (\mu_B) between 200 - 20 MeV. Our measurements of the products \kappa \sigma^2 and S \sigma, which can be related to theoretical calculations sensitive to baryon number susceptibilities and long range correlations, are constant as functions of collision centrality. We compare these products with results from lattice QCD and various models without a critical point and study the \sqrt(s_NN) dependence of \kappa \sigma^2. From the measurements at the three beam energies, we find no evidence for a critical point in the QCD phase diagram for \mu_B below 200 MeV.
Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions from Lattice QCD Calculations.
A search for light long-lived neutral particles with masses in the $O$(MeV-GeV) range is presented. The analysis targets the production of long-lived dark photons in the decay of a Higgs boson produced via gluon-gluon fusion or in association with a $W$ boson. Events that contain displaced collimated Standard Model fermions reconstructed in the calorimeter or muon spectrometer are selected in 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the LHC. Background estimates for contributions from Standard Model processes and instrumental effects are extracted from data. The observed event yields are consistent with the expected background. Exclusion limits are reported on the production cross-section times branching fraction as a function of the mean proper decay length $c\tau$ of the dark photon, or as a function of the dark-photon mass and kinetic mixing parameter that quantifies the coupling between the Standard Model and potential hidden (dark) sectors. A Higgs boson branching fraction above 1% is excluded at 95% CL for a Higgs boson decaying into two dark photons for dark-photon mean proper decay lengths between 10 mm and 250 mm and dark photons with masses between 0.4 GeV and 2 GeV.
Efficiency of the cosmic-ray tagger as function of the γ<sub>d</sub> transverse decay length. The efficiency is calculated accepting the μDPJs for which the cosmic-ray tagger score is > 0.2 for each associated MS-only track.
Measurements of the midrapidity transverse energy distribution, $d\Et/d\eta$, are presented for $p$$+$$p$, $d$$+$Au, and Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV and additionally for Au$+$Au collisions at $\sqrt{s_{_{NN}}}=62.4$ and 130 GeV. The $d\Et/d\eta$ distributions are first compared with the number of nucleon participants $N_{\rm part}$, number of binary collisions $N_{\rm coll}$, and number of constituent-quark participants $N_{qp}$ calculated from a Glauber model based on the nuclear geometry. For Au$+$Au, $\mean{d\Et/d\eta}/N_{\rm part}$ increases with $N_{\rm part}$, while $\mean{d\Et/d\eta}/N_{qp}$ is approximately constant for all three energies. This indicates that the two component ansatz, $dE_{T}/d\eta \propto (1-x) N_{\rm part}/2 + x N_{\rm coll}$, which has been used to represent $E_T$ distributions, is simply a proxy for $N_{qp}$, and that the $N_{\rm coll}$ term does not represent a hard-scattering component in $E_T$ distributions. The $dE_{T}/d\eta$ distributions of Au$+$Au and $d$$+$Au are then calculated from the measured $p$$+$$p$ $E_T$ distribution using two models that both reproduce the Au$+$Au data. However, while the number-of-constituent-quark-participant model agrees well with the $d$$+$Au data, the additive-quark model does not.
dE_T/deta normalized by the number of participant pairs as a function of the number of participants.
Differential cross sections for the reaction $\gamma p \to p \pi^0$ have been measured with the CEBAF Large Acceptance Spectrometer (CLAS) and a tagged photon beam with energies from 0.675 to 2.875 GeV. The results reported here possess greater accuracy in the absolute normalization than previous measurements. They disagree with recent CB-ELSA measurements for the process at forward scattering angles. Agreement with the SAID and MAID fits is found below 1 GeV. The present set of cross sections has been incorporated into the SAID database, and exploratory fits have been extended to 3 GeV. Resonance couplings have been extracted and compared to previous determinations.
Differential cross section for indicent photon energy 1725 MeV.
Beam asymmetry and differential cross section for the reaction gamma+p->eta+p were measured from production threshold to 1500 MeV photon laboratory energy. The two dominant neutral decay modes of the eta meson, eta->2g and eta->3pi0, were analyzed. The full set of measurements is in good agreement with previously published results. Our data were compared with three models. They all fit satisfactorily the results but their respective resonance contributions are quite different. The possible photoexcitation of a narrow state N(1670) was investigated and no evidence was found.
Differential cross section for photon energy 818 MeV as a function of the cosine of the ETA centre of mass angle.
We report measurements of the ratios K+π+, pπ+, K−π−, p¯π−, π−π+, K−K+, and p¯p for hadrons with 0.19<xt<0.62 produced in p−Be and p−W collisions at s=38.8 GeV. The K+π+ ratio at high xt gives the fragmentation-function ratio DuK+Duπ+ at high z. The high-xt K−π− ratio gives an upper limit for DdK−Ddπ− at high z. The pt dependence of pπ+ suggests that scattered constituent diquarks are the primary source of protons with pt<6 GeV/c. We also present species correlations in high-mass h+h− pairs. Strong K+K− and pp¯ correlations were observed.
No description provided.
Experimental results on the production of dimuons by 800-GeV protons incident on a copper target are presented. The results include measurements of both the continuum of dimuons and the dimuon decays of the three lowest-mass ϒ S states. A description of the apparatus, data acquisition, and analysis techniques is included. A comparison of the results with data taken at lower incident energies indicates a scaling behavior of the continuum dimuon yields.
Invariant di-muon cross section for the UPSILON regions (9.36 to 9.54), (9.92 to 10.12), and (10.26 to 10.48) GeV summed with the continuum subtracted.
Results on the channels K − p → Λ 0 η 0 , Λ 0 π 0 , Σ 0 π 0 , Λ 0 π 0 π 0 and Σ 0 π 0 π 0 are obtained in a K − p formation experiment using 1 million photographs taken in a heavy liquid bubble chamber filled with a CF 3 BrC 3 H 8 mixture. The results are compared with hydrogen bubble chamber (HBC) experiments and with experiments having full or partial gamma-ray detection. Our Λ 0 π 0 and Λ 0 + neutral cross section agree with HBC results. Our Σ 0 π 0 cross section does not exhibit a bump at 1670 MeV as previously seen in HBC experiments. Our Λ 0 π 0 π 0 data are dominated by a Σ (1385) π 0 production. Our Σ 0 π 0 π 0 data is consistent with the presence of some Σ (1405) π 0 production.
No description provided.
We report on the first measurement of the triangular $v_3$, quadrangular $v_4$, and pentagonal $v_5$ charged particle flow in Pb-Pb collisions at 2.76 TeV measured with the ALICE detector at the CERN Large Hadron Collider. We show that the triangular flow can be described in terms of the initial spatial anisotropy and its fluctuations, which provides strong constraints on its origin. In the most central events, where the elliptic flow $v_2$ and $v_3$ have similar magnitude, a double peaked structure in the two-particle azimuthal correlations is observed, which is often interpreted as a Mach cone response to fast partons. We show that this structure can be naturally explained from the measured anisotropic flow Fourier coefficients.
v2{SP,Deltaeta=1.0} (blue open circles).
A measurement of the transverse momentum spectra of jets in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV is reported. Jets are reconstructed from charged particles using the anti-$k_{\rm T}$ jet algorithm with jet resolution parameters $R$ of $0.2$ and $0.3$ in pseudo-rapidity $|\eta|<0.5$. The transverse momentum $p_{\rm T}$ of charged particles is measured down to $0.15$ GeV/$c$ which gives access to the low $p_{\rm T}$ fragments of the jet. Jets found in heavy-ion collisions are corrected event-by-event for average background density and on an inclusive basis (via unfolding) for residual background fluctuations and detector effects. A strong suppression of jet production in central events with respect to peripheral events is observed. The suppression is found to be similar to the suppression of charged hadrons, which suggests that substantial energy is radiated at angles larger than the jet resolution parameter $R=0.3$ considered in the analysis. The fragmentation bias introduced by selecting jets with a high $p_{\rm T}$ leading particle, which rejects jets with a soft fragmentation pattern, has a similar effect on the jet yield for central and peripheral events. The ratio of jet spectra with $R=0.2$ and $R=0.3$ is found to be similar in Pb-Pb and simulated PYTHIA pp events, indicating no strong broadening of the radial jet structure in the reconstructed jets with $R<0.3$.
Nuclear modification factor, constructed as the ratio of jet pT spectra in central and peripheral collisions normalized by the nuclear overlap functions, for charged jets with either R = 0.2 or R = 0.3 and a leading charged particle with pT > 5 GeV. Central collisions are defined to have centrality 10-30% and peripheral collisions are defined to have centrality 50-80%. The two systematic uncertainties correspond to the shape uncertainty and the correlated uncertainty.
This report reviews the experimental investigation of high energy e + e − interactions by the MARK J collaboration at PETRA, the electron-positron colliding beam accelerator at DESY in Hamburg, Germany. The physics objectives include studies of several purely electromagnetic processes and hadronic final states, which further our knowledge of the nature of the fundamental constituents and of their strong, electromagnetic and weak interactions. Before discussing the physics results, the main features and the principal components of the MARK J detector are discussed in terms of design, function, and performance. Several aspects of the on-line data collection and the off-line analysis are also outlined. Results are presented on tests of quantum electrodynamics using e + e − → e + e − , μ + μ − and τ + τ − , on the measurement of R , the ratio of the hadronic to the point-like muon pair cross section, on the search for new quark flavors, on the discovery of three jet events arising from the radiation of hard noncollinear gluons as predicted by quantum chromodynamics, and on the determination of the strong coupling constant α s .
MEAN THRUST AND THRUST DISTRIBUTION (1/N)*DN/DTHRUST AT 13, 17, 22 AND 30 GEV. SOMEWHAT DETECTOR DEPENDENT. INCLUDES RED = 1079 AND 1072. SEE ALSO RED = 1114. ALSO JET ANALYSIS USING FOX-WOLFRAM MOMENTS.
We report measurements of the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from a proton target using the CLAS detector at the Thomas Jefferson National Accelerator Facility. The separated structure functions $\sigma_T$, $\sigma_L$, $\sigma_{TT}$, and $\sigma_{LT}$ were extracted from the $\Phi$- and $\epsilon$-dependent differential cross sections taken with electron beam energies of 2.567, 4.056, and 4.247 GeV. This analysis represents the first $\sigma_L/\sigma_T$ separation with the CLAS detector, and the first measurement of the kaon electroproduction structure functions away from parallel kinematics. The data span a broad range of momentum transfers from $0.5\leq Q^2\leq 2.8$ GeV$^2$ and invariant energy from $1.6\leq W\leq 2.4$ GeV, while spanning nearly the full center-of-mass angular range of the kaon. The separated structure functions reveal clear differences between the production dynamics for the $\Lambda$ and $\Sigma^0$ hyperons. These results provide an unprecedented data sample with which to constrain current and future models for the associated production of strangeness, which will allow for a better understanding of the underlying resonant and non-resonant contributions to hyperon production.
Cross sections for incident energy 4 GeV for the Q**2 range 0.9 to 1.3 GeV**2 and W range 2.2 to 2.3 GeV.
Polarization and differential cross-section data for elastic scattering of positive pions on protons between 0.82 and 2.74 GeV/ c are presented. A dip in the polarization, at constant u ≈ −0.65 GeV 2 , is observed. The data are compared with published phase-shift analyses.
No description provided.
Polarization distributions and differential cross section data for elastic scattering of negative pions on protons between 865 and 2732 MeV/ c are presented. They are compared with published phase-shift analyses.
No description provided.
Total and differential cross sections for π−p elastic scattering are presented at 35 energies between 1400 and 2000 MeV.
No description provided.
The excitation of theΔ resonance is observed in proton collisions on C, Nb and Pb targets at 0.8 and 1.6 GeV incident energies. The mass E0 and widthΓ of the resonance are determined from the invariant mass spectra of correlated (p, π±)-pairs in the final state of the collision: The mass E0 is smaller than that of the free resonance, however by comparing to intra-nuclear cascade calculations, this reduction is traced back to the effects of Fermi motion, NN scattering and pion reabsorption in nuclear matter.
.
In this paper, results are presented from a study of the hadronic final states in e+e− annihilation at 29 GeV. The data were obtained with the High Resolution Spectrometer (HRS) at the SLAC PEP e+e− colliding-beam facility. The results are based on 6342 selected events corresponding to an integrated luminosity of 19.6 pb−1. The distributions of the events in sphericity (S), thrust (T), and aplanarity (A) are given and compared to other e+e− data in the same energy range. We measure 〈S〉=0.130±0.003±0.010 and 〈1-T〉=0.100±0.002. The sphericity distribution is compared to sphericity measurements made for beam jets in hadronic collisions as well as jets studied in neutrino scattering. The data sample is further reduced to 4371 events with the two-jet selections, S≤0.25 and A≤0.1. The single-particle distributions in the longitudinal and transverse directions are given. For low values of the momentum fraction (z=2p/W), the invariant distribution shows a maximum at z∼0.06, consistent with a QCD expectation. The data at high Feynman x (xF) show distribution consistent with being dominated by a (1-xf)2 variation for the leading quark-meson transition. The rapidity distribution shows a shallow central minimum with a height (1/NevdNh/dY‖Y=0=2.3±0.02±0.07. The mean charged multiplicity is measured to be 〈nch〉=13.1±0.05±0.6. The mean transverse momentum relative to the thrust axis 〈pT〉 rises as a function of z to a value of 0.70±0.02 GeV/c for z≳0.3. The distributions are compared to those measured in other reactions.
No description provided.
None
No description provided.
Results from a high-statistics experiment involving an exposure of the SLAC 82-in. hydrogen bubble chamber to a beam of 8-GeV/c π− yielding a final state of π−π+π−p are presented. Copious production of ρ, Δ++, and f is found. Considerable quasi-two-body production in which one particle decays to one of the above resonances is also observed. Some double-resonance production involving baryon and meson resonances is also seen. The production properties of ρ, Δ++, and f mesons are well described by a double-Regge model.
No description provided.
The polarized longitudinal-transverse structure function $\sigma_{LT^\prime}$ measures the interference between real and imaginary amplitudes in pion electroproduction and can be used to probe the coupling between resonant and non-resonant processes. We report new measurements of $\sigma_{LT^\prime}$ in the $N(1440){1/2}^+$ (Roper) resonance region at $Q^2=0.40$ and 0.65 GeV$^2$ for both the $\pi^0 p$ and $\pi^+ n$ channels. The experiment was performed at Jefferson Lab with the CEBAF Large Acceptance Spectrometer (CLAS) using longitudinally polarized electrons at a beam energy of 1.515 GeV. Complete angular distributions were obtained and are compared to recent phenomenological models. The $\sigma_{LT^\prime}(\pi^+ n)$ channel shows a large sensitivity to the Roper resonance multipoles $M_{1-}$ and $S_{1-}$ and provides new constraints on models of resonance formation.
Polarized structure function of the reaction E- P --> E- PI0 P for Q**2 = 0.40 and W = 1.34 GeV.
The exclusive omega electroproduction off the proton was studied in a large kinematical domain above the nucleon resonance region and for the highest possible photon virtuality (Q2) with the 5.75 GeV beam at CEBAF and the CLAS spectrometer. Cross sections were measured up to large values of the four-momentum transfer (-t < 2.7 GeV2) to the proton. The contributions of the interference terms sigma_TT and sigma_TL to the cross sections, as well as an analysis of the omega spin density matrix, indicate that helicity is not conserved in this process. The t-channel pi0 exchange, or more generally the exchange of the associated Regge trajectory, seems to dominate the reaction gamma* p -> omega p, even for Q2 as large as 5 GeV2. Contributions of handbag diagrams, related to Generalized Parton Distributions in the nucleon, are therefore difficult to extract for this process. Remarkably, the high-t behaviour of the cross sections is nearly Q2-independent, which may be interpreted as a coupling of the photon to a point-like object in this kinematical limit.
Differential cross sections DSIG/DT for Q**2 = 2.371 GeV**2 and W = 1.85 GeV.
A new measurement of the proton structure function $F_2(x,Q~2)$ is reported for momentum transfers squared $Q~2$ between 1.5GeV$~2$ and 5000GeV$~2$ and for Bjorken $x$ between $3\cdot 10~{-5}$ and $0.32$ using data collected by the HERA experiment H1 in 1994. The data represent an increase in statistics by a factor of ten with respect to the analysis of the 1993 data. Substantial extension of the kinematic range towards low $Q~2$ and $x$ has been achieved using dedicated data samples and events with initial state photon radiation. The structure function is found to increase significantly with decreasing $x$, even in the lowest accessible $Q~2$ region. The data are well described by a Next to Leading Order QCD fit and the gluon density is extracted.
Data from normal vertex sample.
Exclusive production of $\rho^0$ and $J/\psi$ mesons in e^+ p collisions has been studied with the ZEUS detector in the kinematic range $0.25 < Q^2 < 50 GeV^2, 20 < W < 167 GeV$ for the $\rho^0$ data and $2 < Q^2 < 40 GeV^2, 50 < W < 150 GeV$ for the $J/\psi$ data. Cross sections for exclusive $\rho^0$ and $J/\psi$ production have been measured as a function of $Q^2, W$ and $t$. The spin-density matrix elements $r^{04}_{00}, r^1_{1-1}$ and $Re r^{5}_{10}$ have been determined for exclusive $\rho^0$ production as well as $r^{04}_{00}$ and $r^{04}_{1-1}$ for exclusive $J/\psi$ production. The results are discussed in the context of theoretical models invoking soft and hard phenomena.
The spin-density martix elements deletermined for various values of W and Q**2 for the RHO0 BPC sample.
The shapes of jets with transverse energies, E_T(jet), up to 45 GeV produced in neutral- and charged-current deep inelastic e+p scattering (DIS) at Q**2 > 100 GeV**2 have been measured with the ZEUS detector at HERA. Jets are identified using a cone algorithm in the eta-phi plane with a cone radius of one unit. The jets become narrower as E_T(jet) increases. The jet shapes in neutral- and charged-current DIS are found to be very similar. The jets in neutral-current DIS are narrower than those in resolved processes in photoproduction and closer to those in direct-photon processes for the same ranges in E_T(jet) and jet pseudorapidity. The jet shapes in DIS are observed to be similar to those in e+e- interactions and narrower than those in pbarp collisions for comparable E_T(jet). Since the jets in e+e- interactions and e+p DIS are predominantly quark initiated in both cases, the similarity in the jet shapes indicates that the pattern of QCD radiation within a quark jet is to a large extent independent of the hard scattering process in these reactions.
Comparison of the differential jet shape with those from E+E- interactions obtained in a comparable data from OPAL (Alees et al. ZP C63 (94) 197).
Low x deep-inelastic ep scattering data, taken in 1994 at the H1 detector at HERA, are analysed in the Breit frame of reference. The evolution of the peak and width of the current hemisphere fragmentation function is presented as a function of Q and compared with e+e- results at equivalent centre of mass energies. Differences between the average charged multiplicity and the multiplicity of e+e- annihilations at low energies are analysed. Invariant energy spectra are compared with MLLA predictions. Distributions of multiplicity are presented as functions of Bjorken-x and Q^2, and KNO scaling is discussed.
The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 6.20 GeV, X=0.00158).
The DIS diffractive cross section, $d\sigma^{diff}_{\gamma^* p \to XN}/dM_X$, has been measured in the mass range $M_X < 15$ GeV for $\gamma^*p$ c.m. energies $60 < W < 200$ GeV and photon virtualities $Q^2 = 7$ to 140 GeV$^2$. For fixed $Q^2$ and $M_X$, the diffractive cross section rises rapidly with $W$, $d\sigma^{diff}_{\gamma^*p \to XN}(M_X,W,Q^2)/dM_X \propto W^{a^{diff}}$ with $a^{diff} = 0.507 \pm 0.034 (stat)^{+0.155}_{-0.046}(syst)$ corresponding to a $t$-averaged pomeron trajectory of $\bar{\alphapom} = 1.127 \pm 0.009 (stat)^{+0.039}_{-0.012} (syst)$ which is larger than $\bar{\alphapom}$ observed in hadron-hadron scattering. The $W$ dependence of the diffractive cross section is found to be the same as that of the total cross section for scattering of virtual photons on protons. The data are consistent with the assumption that the diffractive structure function $F^{D(3)}_2$ factorizes according to $\xpom F^{D(3)}_2 (\xpom,\beta,Q^2) = (x_0/ \xpom)^n F^{D(2)}_2(\beta,Q^2)$. They are also consistent with QCD based models which incorporate factorization breaking. The rise of $\xpom F^{D(3)}_2$ with decreasing $\xpom$ and the weak dependence of $F^{D(2)}_2$ on $Q^2$ suggest a substantial contribution from partonic interactions.
Diffractive structure function F2(D3).
The transition between photoproduction and deep-inelastic scattering is investigated in jet production at the HERA ep collider, using data collected by the H1 experiment. Measurements of the differential inclusive jet cross-sections dsigep/dEt* and dsigmep/deta*, where Et* and eta* are the transverse energy and the pseudorapidity of the jets in the virtual photon-proton centre of mass frame, are presented for 0 < Q2 < 49 GeV2 and 0.3 < y < 0.6. The interpretation of the results in terms of the structure of the virtual photon is discussed. The data are best described by QCD calculations which include a partonic structure of the virtual photon that evolves with Q2.
The inclusive virtual photon-proton jet cross section.
Transverse momentum spectra of charged particles produced in deep inelastic scattering are measured as a function of the kinematic variables x_B and Q2 using the H1 detector at the ep collider HERA. The data are compared to different parton emission models, either with or without ordering of the emissions in transverse momentum. The data provide evidence for a relatively large amount of parton radiation between the current and the remnant systems.
Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.
Dijet cross sections are presented using photoproduction data obtained with the ZEUS detector during 1994. These measurements represent an extension of previous results, as the higher statistics allow cross sections to be measured at higher jet transverse energy (ETJ). Jets are identified in the hadronic final state using three different algorithms, and the cross sections compared to complete next-to-leading order QCD calculations. Agreement with these calculations is seen for the pseudorapidity dependence of the direct photon events with ETJ > 6 GeV and of the resolved photon events with ETJ > 11 GeV. Calculated cross sections for resolved photon processes with 6 GeV < ETJ < 11 GeV lie below the data.
Dijet cross section using the KTCLUS jet alogrithm with a minimum ET for each jet of 8 GeV and a requirement on X(NAME=GAMMA_OBS) to be > 0.75. The second DSYS errors are the correlated uncertainties.
The production of D*+-(2010) mesons in deep inelastic scattering has been measured in the ZEUS detector at HERA using an integrated luminosity of 37 pb^-1. The decay channels D*+ -> D0 pi+(+c.c.), with D0 -> K- pi+ or D0 ->K- pi- pi+ pi+, have been used to identify the D mesons. The e+p cross section for inclusive D*+- production with 1<Q^2<600 GeV^2 and 0.02<y<0.7 is 8.31 +- 0.31(stat.) +0.30-0.50(syst.) nb in the kinematic region 1.5< pT(D*+-)<15 GeV and |eta(D*+-)|<1.5. Differential cross sections are consistent with a next-to-leading-order perturbative-QCD calculation when using charm-fragmentation models which take into account the interaction of the charm quark with the proton remnant. The observed cross section is extrapolated to the full kinematic region in pT(D*+-) and eta(D*+-) in order to determine the charm contribution, F^ccbar_2(x,Q^2), to the proton structure function. The ratio F^ccbar_2/F_2 rises from ~10% at Q^2 ~1.8 GeV^2 to ~30% at Q^2 ~130 GeV^2 for x values in the range 10^-4 to 10-3.
The charmed structure function F2(C=CHARM) derived from a combination of the K2PI and K4PI data. There are additional systematic uncertainties described in the text of the paper which include the 1.65 PCT luminosity uncertainty and a 9 PCT uncertainty in the charm hadronization fraction to D*+-.
Deep-inelastic ep scattering data, taken with the H1 detector at HERA, are used to study the event shape variables thrust, jet broadening, jet mass, C parameter and two kinds of differential two-jet rate. The data cover a large range of the four-momentum transfer Q, which is considered to be the relevant energy scale, between 7 GeV and 100 GeV. The Q dependences of the mean values are compared with second order calculations of perturbative QCD applying power law corrections proportional to 1/Q^p to account for hadronization effects. The concept of power corrections is investigated by fitting simultaneously a non-perturbative parameter alpha_p and the strong coupling constant alpha_s.
Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).
The cross section for dijet photoproduction at high transverse energies is presented as a function of the transverse energies and the pseudorapidities of the jets. The measurement is performed using a sample of ep-interactions corresponding to an integrated luminosity of 6.3 pb^(-1), recorded by the ZEUS detector.Jets are defined by applying a k_T-clustering algorithm to the hadrons observed in the final state. The measured cross sections are compared to next-to-leading order QCD calculations. In a kinematic regime where theoretical uncertainties are expected to be small, the measured cross sections are higher than these calculations.
The dijet cross section for the x(gamma)>0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
We present a study of the production of K_s^0 and Lambda^0 in inelastic pbar-p collisions at sqrt(s)= 1800 and 630 GeV using data collected by the CDF experiment at the Fermilab Tevatron. Analyses of K_s^0 and Lambda^0 multiplicity and transverse momentum distributions, as well as of the dependencies of the average number and <p_T> of K_s^0 and Lambda^0 on charged particle multiplicity are reported. Systematic comparisons are performed for the full sample of inelastic collisions, and for the low and high momentum transfer subsamples, at the two energies. The p_T distributions extend above 8 GeV/c, showing a <p_T> higher than previous measurements. The dependence of the mean K_s^0(Lambda^0) p_T on the charged particle multiplicity for the three samples shows a behavior analogous to that of charged primary tracks.
Average PT of LAMBDA at a centre of mass 630 GeV for the SOFT data sample.
Photoproduction of the cascade resonances has been investigated in the reactions $\gamma p \to K^+ K^+ (X)$ and $\gamma p \to K^+ K^+ \pi^- (X)$. The mass split of the $\Xi$ doublet is measured to be $5.4\pm 1.8$ MeV/c$^2$, consistent with existing measurements. The differential (total) cross sections for the $\Xi^{-}$ have been determined for photon beam energies from 2.75 to 3.85 (4.75) GeV, and are consistent with a possible production mechanism of $Y^*\to K^+\Xi^-$ through a $t$-channel process. The reaction $\gamma p \to K^+ K^+ \pi^-[\Xi^0]$ has also been investigated in search of excited cascade resonances. No significant signal of excited cascade states other than the $\Xi^-(1530)$ is observed. The cross section results of the $\Xi^-(1530)$ have also been obtained for photon beam energies from 3.35 to 4.75 GeV.
Differential cross section for XI- production as a function of the invariant mass of the K+ meson pair for incident photon energy 3.79 Gev.
Spin transfer from circularly polarized real photons to recoiling hyperons has been measured for the reactions $\vec\gamma + p \to K^+ + \vec\Lambda$ and $\vec\gamma + p \to K^+ + \vec\Sigma^0$. The data were obtained using the CLAS detector at Jefferson Lab for center-of-mass energies $W$ between 1.6 and 2.53 GeV, and for $-0.85<\cos\theta_{K^+}^{c.m.}< +0.95$. For the $\Lambda$, the polarization transfer coefficient along the photon momentum axis, $C_z$, was found to be near unity for a wide range of energy and kaon production angles. The associated transverse polarization coefficient, $C_x$, is smaller than $C_z$ by a roughly constant difference of unity. Most significantly, the {\it total} $\Lambda$ polarization vector, including the induced polarization $P$, has magnitude consistent with unity at all measured energies and production angles when the beam is fully polarized. For the $\Sigma^0$ this simple phenomenology does not hold. All existing hadrodynamic models are in poor agreement with these results.
Coefficients Cx and Cz for the reaction GAMMA P --> K+ SIGMA0 for incident energy = 1.534 GeV and W = 1.939 GeV.
Production of multi-strange baryons and antibaryons is expected to be a useful indicator in the search for Quark-Gluon Plasma formation. Production of Ξ − and Ξ − has been observed for the first time in ultra-relativistic heavy ion interactions by the WA85 Experiment. We describe the procedure used to select these cascade candidates and show that Ξ − and Ξ − decays can be identified. Preliminary ratios of Ξ/Ξ production in sulphur-tungsten and proton-tungsten interactions are also presented.
PRODUCTION AT CENTRAL RAPIDITY. 82 XI- AND 22 XIBAR+ CANDIDATES.
Internal jet structure in dijet production in deep-inelastic scattering is measured with the H1 detector at HERA. Jets with transverse energies ET,Breit > 5 GeV are selected in the Breit frame employing k_perp and cone jet algorithms. In the kinematic region of squared momentum transfers 10 < Q2 <~ 120 GeV2 and x-Bjorken values 2.10^-4 <~ xBj <~ 8.10^-3, jet shapes and subjet multiplicities are measured as a function of a resolution parameter. Distributions of both observables are corrected for detector effects and presented as functions of the transverse jet energy and jet pseudo-rapidity. Dependences of the jet shape and the average number of subjets on the transverse energy and the pseudo-rapidity of the jet are observed. With increasing transverse jet energies and decreasing pseudo-rapidities, i.e.towards the photon hemisphere, the jets are more collimated. QCD models give a fair description of the data.
The average number of subjets as a function of the resolution parameter YCUT using the inclusive KT jet finding algorithm in the pseudorapidity range < 1.5 and the ET range > 8 GeV YCUT using the inclusive KT jet finding algorithm.
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