We present a measurement of the cross sections for the associated production of a $W$ boson with at least one heavy quark jet, $b$ or $c$, in proton-antiproton collisions. Data corresponding to an integrated luminosity of 8.7 fb$^{-1}$ recorded with the D0 detector at the Fermilab Tevatron \ppbar Collider at $\sqrt{s}=1.96$ TeV are used to measure the cross sections differentially as a function of the jet transverse momenta in the range 20 to 150 GeV. These results are compared to calculations of perturbative QCD theory as well as predictions from Monte Carlo generators.
The $W + b$-jet production cross sections times $W \to \mu\nu$ branching fraction, ${\rm d}\sigma/{\rm d}p_T^{\rm jet}$.
The $W + c$-jet production cross sections times $W \to \mu\nu$ branching fraction, ${\rm d}\sigma/{\rm d}p_T^{\rm jet}$.
The $\sigma(W+c)/\sigma(W+b)$ cross section ratio in bins of $c(b)$-jet $p_T$.
Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3 fb$^{-1}$ of $pp$ collisions produced by the Large Hadron Collider at a center-of-mass energy of $\sqrt{s} = 8$ TeV and recorded by the ATLAS detector. Cross sections are obtained from measured $H \rightarrow \gamma \gamma$ and $H \rightarrow ZZ ^{*}\rightarrow 4\ell$ event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be $\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}$. The measurements are compared to state-of-the-art predictions.
Measured cross section in bins of $p_{\rm{T}}^{\rm{H}}$.
Measured cross section in bins of $|y^{\rm{H}}|$.
Measured cross section in bins of $N_{\rm{jets}}$.
This paper presents a measurement of the double-differential cross section for the Drell-Yan $Z/\gamma^{*} \rightarrow \ell^{+} \ell^{-}$ and photon-induced $\gamma\gamma \rightarrow \ell^{+} \ell^{-}$ processes where $\ell$ is an electron or muon. The measurement is performed for invariant masses of the lepton pairs, $m_{\ell\ell}$, between 116 GeV and 1500 GeV, using a sample of 20.3 fb$^{-1}$ of pp collisions data at centre-of-mass energy of $\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the LHC in 2012. The data are presented double differentially in invariant mass and absolute dilepton rapidity as well as in invariant mass and absolute pseudorapidity separation of the lepton pair. The single-differential cross section as a function of $m_{\ell\ell}$ is also reported. The electron and muon channel measurements are combined and a total experimental precision of better than 1% is achieved at low $m_{\ell\ell}$. A comparison to next-to-next-to-leading order perturbative QCD predictions using several recent parton distribution functions and including next-to-leading order electroweak effects indicates the potential of the data to constrain parton distribution functions. In particular, a large impact of the data on the photon PDF is demonstrated.
The combined Born-level single-differential cross section as a function of invariant mass. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".
The combined Born-level double-differential cross section as a function of invariant mass and absolute rapidity. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".
The combined Born-level double-differential cross section as a function of invariant mass and absolute pseudorapidity separation of the leptons. The measurements are listed together with the statistical and systematic uncertainties. The systematic uncertainties are separated into one uncorrelated, 35 correlated sources and the luminosity uncertainty. The sign of the uncertainty corresponds to a one standard deviation upward shift of the uncertainty source, where +/- means "+" and -/+ means "-".
The dijet production cross section for jets containing a $b$-hadron ($b$-jets) has been measured in proton-proton collisions with a centre-of-mass energy of $\sqrt{s} = 7$ TeV, using the ATLAS detector at the LHC. The data used correspond to an integrated luminosity of 4.2 fb$^{-1}$. The cross section is measured for events with two identified $b$-jets with a transverse momentum $p_T > 20$ GeV and a minimum separation in the $\eta$-$\phi$ plane of $\Delta R = 0.4$. At least one of the jets in the event is required to have $p_T > 270$ GeV. The cross section is measured differentially as a function of dijet invariant mass, dijet transverse momentum, boost of the dijet system, and the rapidity difference, azimuthal angle and angular distance between the $b$-jets. The results are compared to different predictions of leading order and next-to-leading order perturbative quantum chromodynamics matrix elements supplemented with models for parton-showers and hadronization.
Results for the m_bb distribution. Statistical and systematic uncertainties are quoted.
Results for the DeltaPhi distribution. Statistical and systematic uncertainties are quoted.
Results for the y* distribution. Statistical and systematic uncertainties are quoted.
A measurement of the total $pp$ cross section at the LHC at $\sqrt{s}=8$ TeV is presented. An integrated luminosity of $500$ $\mu$b$^{-1}$ was accumulated in a special run with high-$\beta^{\star}$ beam optics to measure the differential elastic cross section as a function of the Mandelstam momentum transfer variable $t$. The measurement is performed with the ALFA sub-detector of ATLAS. Using a fit to the differential elastic cross section in the $-t$ range from $0.014$ GeV$^2$ to $0.1$ GeV$^2$ to extrapolate $t\rightarrow 0$, the total cross section, $\sigma_{\mathrm{tot}}(pp\rightarrow X)$, is measured via the optical theorem to be: $\sigma_{\mathrm{tot}}(pp\rightarrow X) = {96.07} \; \pm 0.18 \; ({{stat.}}) \pm 0.85 \; ({{exp.}}) \pm 0.31 \; ({extr.}) \; {mb} \;,$ where the first error is statistical, the second accounts for all experimental systematic uncertainties and the last is related to uncertainties in the extrapolation $t\rightarrow 0$. In addition, the slope of the exponential function describing the elastic cross section at small $t$ is determined to be $B = 19.74 \pm 0.05 \; ({{stat.}}) \pm 0.23 \; ({{syst.}}) \; {GeV}^{-2}$.
The measured total cross section, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t-->0.
The nuclear slope of the differential eslastic cross section at small |t|, the first systematic error accounts for all experimental uncertainties and the second error for the extrapolation t-->0.
The total elastic cross section and the observed elastic cross section within the fiducial volume.
The $W$ boson angular distribution in events with high transverse momentum jets is measured using data collected by the ATLAS experiment from proton-proton collisions at a centre-of-mass energy $\sqrt{s}=$ 8 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 20.3 fb$^{-1}$. The focus is on the contributions to $W$ + jets processes from real $W$ emission, which is achieved by studying events where a muon is observed close to a high transverse momentum jet. At small angular separations, these contributions are expected to be large. Various theoretical models of this process are compared to the data in terms of the absolute cross-section and the angular distributions of the muon from the leptonic $W$ decay.
Measured integrated cross-sections as a function of leading jet transverse momentum for the collinear region ($0.2 < \Delta R < 2.4$), the back-to-back region ($\Delta R > 2.4$) and inclusively.
Measured cross-section as a function of angular separation between the muon and the closest jet. Multiplicative correction factors for using prompt muons and prompt dressing photons in the particle-level selection, derived from ALPGEN 2.14 interfaced with PYTHIA 6.426, are also shown.
Breakdown of uncertainties in percent.
Inclusive four-jet events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV are analysed for the presence of hard double-parton scattering using data corresponding to an integrated luminosity of 37.3 pb$^{-1}$, collected with the ATLAS detector at the LHC. The contribution of hard double-parton scattering to the production of four-jet events is extracted using an artificial neural network, assuming that hard double-parton scattering can be approximated by an uncorrelated overlaying of dijet events. For events containing at least four jets with transverse momentum $p_{\mathrm{T}} \geq 20$ GeV and pseudorapidity $\eta \leq 4.4$, and at least one having $p_{\mathrm{T}} \geq 42.5$ GeV, the contribution of hard double-parton scattering is estimated to be $f_{\mathrm{DPS}} = 0.092 ^{+0.005}_{-0.011} (\mathrm{stat.}) ^{+0.033}_{-0.037} (\mathrm{syst.})$. After combining this measurement with those of the inclusive dijet and four-jet cross-sections in the appropriate phase space regions, the effective overlap area between the interacting protons, $\sigma_{\mathrm{eff}}$, was determined to be $\sigma_{\mathrm{eff}} = 14.9 ^{+1.2}_{-1.0} (\mathrm{stat.}) ^{+5.1}_{-3.8} (\mathrm{syst.})$ mb. This result is consistent within the quoted uncertainties with previous measurements of $\sigma_{\mathrm{eff}}$, performed at centre-of-mass energies between 63 GeV and 8 TeV using various final states, and it corresponds to $21^{+7}_{-6}$% of the total inelastic cross-section measured at $\sqrt{s} = 7$ TeV. The distributions of the observables sensitive to the contribution of hard double-parton scattering, corrected for detector effects, are also provided.
Normalized distribution of the variable $\Delta^{p_{\mathrm{T}}}_{34}$, defined in Eq (16) of the paper, in data after unfolding to particle level.
Normalized distribution of the variable $\Delta\phi_{34}$, defined in Eq (16) of the paper, in data after unfolding to particle level.
Normalized distribution of the variable $\Delta^{p_{\mathrm{T}}}_{12}$, defined in Eq (16) of the paper, in data after unfolding to particle level.
This paper describes a measurement of fiducial and differential cross sections of gluon-fusion Higgs boson production in the $H{\rightarrow\,}WW^{\ast}{\rightarrow\,}e\nu\mu\nu$ channel, using 20.3 fb$^{-1}$ of proton-proton collision data. The data were produced at a centre-of-mass energy of $\sqrt{s} = 8$ TeV at the CERN Large Hadron Collider and recorded by the ATLAS detector in 2012. Cross sections are measured from the observed $H{\rightarrow\,}WW^{\ast}{\rightarrow\,}e\nu\mu\nu$ signal yield in categories distinguished by the number of associated jets. The total cross section is measured in a fiducial region defined by the kinematic properties of the charged leptons and neutrinos. Differential cross sections are reported as a function of the number of jets, the Higgs boson transverse momentum, the dilepton rapidity, and the transverse momentum of the leading jet. The jet-veto efficiency, or fraction of events with no jets above a given transverse momentum threshold, is also reported. All measurements are compared to QCD predictions from Monte Carlo generators and fixed-order calculations, and are in agreement with the Standard Model predictions.
Measured total fiducial cross section in fb.
Measured fiducial cross section in fb as a function of Njet. Jet PT>25 GeV for |eta|<2.4 and PT>30 GeV for 2.4<|eta|<4.5.
Measured fiducial cross section in fb/GeV as a function of pTH.
A measurement of the correlations between the polar angles of leptons from the decay of pair-produced $t$ and $\bar{t}$ quarks in the helicity basis is reported, using proton-proton collision data collected by the ATLAS detector at the LHC. The dataset corresponds to an integrated luminosity of 4.6fb$^{-1}$ at a center-of-mass energy of $\sqrt{s}=7$TeV collected during 2011. Candidate events are selected in the dilepton topology with large missing transverse momentum and at least two jets. The angles $\theta_1$ and $\theta_2$ between the charged leptons and the direction of motion of the parent quarks in the $t\bar{t}$ rest frame are sensitive to the spin information, and the distribution of {\mbox{$\cos\theta_1\cdot\cos\theta_2$}} is sensitive to the spin correlation between the $t$ and $\bar{t}$ quarks. The distribution is unfolded to parton level and compared to the next-to-leading order prediction. A good agreement is observed.
The numerical summary of the unfolded $\cos\theta_1\cdot\cos\theta_2$ distribution, with statistical and systematic uncertainties.
The correlation factors for the statistical uncertainties between any two bins of the unfolded distribution.
This paper presents measurements of $W^\pm Z$ production in $pp$ collisions at a center-of-mass energy of 8 TeV. The gauge bosons are reconstructed using their leptonic decay modes into electrons and muons. The data were collected in 2012 by the ATLAS experiment at the Large Hadron Collider, and correspond to an integrated luminosity of 20.3 fb$^{-1}$. The measured inclusive cross section in the detector fiducial region is $\sigma_{W^\pm Z \rightarrow \ell^{'} \nu\ \ell \ell} = 35.1 \pm$ 0.9 (stat.) $\pm 0.8$ (sys.) $\pm 0.8$ (lumi.) fb, for one leptonic decay channel. In comparison, the next-to-leading-order Standard Model expectation is 30.0 $\pm$ 2.1 fb. Cross sections for $W^+Z$ and $W^-Z$ production and their ratio are presented as well as differential cross sections for several kinematic observables. Limits on anomalous triple gauge boson couplings are derived from the transverse mass spectrum of the $W^\pm Z$ system. From the analysis of events with a $W$ and a $Z$ boson associated with two or more forward jets an upper limit at 95% confidence level on the $W^\pm Z$ scattering cross section of 0.63 fb, for each leptonic decay channel, is established, while the Standard Model prediction at next-to-leading order is 0.13 fb. Limits on anomalous quartic gauge boson couplings are also extracted.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
A measurement of the production of three isolated photons in proton-proton collisions at a centre-of-mass energy $\sqrt{s}$ = 8 TeV is reported. The results are based on an integrated luminosity of 20.2 fb$^{-1}$ collected with the ATLAS detector at the LHC. The differential cross sections are measured as functions of the transverse energy of each photon, the difference in azimuthal angle and in pseudorapidity between pairs of photons, the invariant mass of pairs of photons, and the invariant mass of the triphoton system. A measurement of the inclusive fiducial cross section is also reported. Next-to-leading-order perturbative QCD predictions are compared to the cross-section measurements. The predictions underestimate the measurement of the inclusive fiducial cross section and the differential measurements at low photon transverse energies and invariant masses. They provide adequate descriptions of the measurements at high values of the photon transverse energies, invariant mass of pairs of photons, and invariant mass of the triphoton system.
The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon1).
The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon2).
The three isolated photons cross section with systematic and statistical uncertainties as a function of ET(Photon3).
Measurements of normalized differential cross-sections of top quark pair ($t\bar t$) production are presented as a function of the mass, the transverse momentum and the rapidity of the $t\bar t$ system in proton-proton collisions at center-of-mass energies of $\sqrt{s}$ = 7 TeV and 8 TeV. The dataset corresponds to an integrated luminosity of 4.6 fb$^{-1}$ at 7 TeV and 20.2 fb$^{-1}$ at 8 TeV, recorded with the ATLAS detector at the Large Hadron Collider. Events with top quark pair signatures are selected in the dilepton final state, requiring exactly two charged leptons and at least two jets with at least one of the jets identified as likely to contain a $b$-hadron. The measured distributions are corrected for detector effects and selection efficiency to cross-sections at the parton level. The differential cross-sections are compared with different Monte Carlo generators and theoretical calculations of $t\bar t$ production. The results are consistent with the majority of predictions in a wide kinematic range.
Parton-level normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system transverse momentum $p_{T, t\bar t}$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
Parton-level normalized $t\bar t$ differential cross-sections for the $t\bar t$ system absolute rapidity $|y_{t\bar t}|$ at $\sqrt{s}$ = 7 TeV. The cross-sections in the last bins include events (if any) beyond of the bin edges. The uncertainties quoted in the second column represent the statistical and systematic uncertainties added in quadrature.
A measurement of the cross section for the inclusive production of isolated prompt photons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 8$ TeV is presented. The measurement covers the pseudo rapidity ranges $|\eta^{\gamma}| < 1.37$ and $1.56 \leq |\eta^{\gamma}| < 2.37$ in the transverse energy range $25 < E_{\rm T}^{\gamma} < 1500$ GeV. The results are based on an integrated luminosity of 20.2 fb$^{-1}$, recorded by the ATLAS detector at the LHC. Photon candidates are identified by combining information from the calorimeters and the inner tracker. The background is subtracted using a data-driven technique, based on the observed calorimeter shower-shape variables and the deposition of hadronic energy in a narrow cone around the photon candidate. The measured cross sections are compared with leading-order and next-to-leading order perturbative QCD calculations and are found to be in a good agreement over ten orders of magnitude.
The inclusive prompt photon cross section with systematic and statistical uncertainties for the region |eta(gamma)| < 0.6.
The inclusive prompt photon cross section with systematic and statistical uncertainties for the region 0.6<|eta(gamma)| < 1.37.
The inclusive prompt photon cross section with systematic and statistical uncertainties for the region 1.56<|eta(gamma)| < 1.81.
The production of $W$ boson pairs in proton-proton collisions at $\sqrt{s}=$ 8 TeV is studied using data corresponding to 20.3 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The $W$ bosons are reconstructed using their leptonic decays into electrons or muons and neutrinos. Events with reconstructed jets are not included in the candidate event sample. A total of 6636 $WW$ candidate events are observed. Measurements are performed in fiducial regions closely approximating the detector acceptance. The integrated measurement is corrected for all acceptance effects and for the $W$ branching fractions to leptons in order to obtain the total $WW$ production cross section, which is found to be 71.1$\pm1.1$(stat)$^{+5.7}_{-5.0}$(syst)$\pm1.4$ pb. This agrees with the next-to-next-to-leading-order Standard Model prediction of 63.2$^{+1.6}_{-1.4}$(scale)$\pm1.2$(PDF) pb. Fiducial differential cross sections are measured as a function of each of six kinematic variables. The distribution of the transverse momentum of the leading lepton is used to set limits on anomalous triple-gauge-boson couplings.
Measured production cross sections of WW production in the fiducial region for different final states corresponding to different W decay channels: both W's decaying into electrons or both decaying to muon. The cross sections are defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)<2.47 and to lie outside of 1.37 < abs(eta) < 1.53, muons are required to lie within abs(eta)<2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 45 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos multiplied by the sine of azimuthal difference between lepton and the vectorial sum of the neutrinos in the event should be larger than 45 GeV if the azimuthal difference between lepton and the vectorial sum of the neutrinos is smaller than PI/2. The invariant mass of the leptons should exceed 15 GeV. The absolute difference between the invariant mass of the leptons and the mass of the Z boson should be larger than 15 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)<4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.
Measured production cross section of WW production in the fiducial region in case one W boson decays into a prompt electron and the other one into a prompt muon. The cross section is defined for direct decays of the W bosons into prompt electrons or muons, intermediate decays into tau leptons are disregarded. The electrons are required to be contained within abs(eta)<2.47 and to lie outside of 1.37 < abs(eta) < 1.53, muons are required to lie within abs(eta)<2.4. The leading and subleading leptons in the events are required to have a transverse momentum above 25 and 20 GeV respectively. The transverse momentum of the vectorial sum of the neutrinos in the event should be larger than 20 GeV (PT(C=SUM(NU))). The transverse momentum of the vectorial sum of the neutrinos is multiplied by the sine of the azimuthal difference between lepton and the vectorial sum of the neutrinos if their azimuthal difference is smaller than PI/2. It is required to be larger than 15 GeV. The invariant mass of the leptons should exceed 10 GeV. Particle-level jets are defined using the anti-kT algorithm with radius of 0.4. No jets above 25 GeV and within abs(eta)<4.5 are allowed in the event. Both, resonant and non-resonant WW production processes, are included in the cross sections.
Measured total production cross sections of WW production in the total phase space. Both, resonant and non-resonant WW, production are considered as signal.
The dynamics of isolated-photon production in association with a jet in proton-proton collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset with an integrated luminosity of 3.2 fb$^{-1}$. Photons are required to have transverse energies above 125 GeV. Jets are identified using the anti-$k_t$ algorithm with radius parameter $R=0.4$ and required to have transverse momenta above 100 GeV. Measurements of isolated-photon plus jet cross sections are presented as functions of the leading-photon transverse energy, the leading-jet transverse momentum, the azimuthal angular separation between the photon and the jet, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system. Tree-level plus parton-shower predictions from SHERPA and PYTHIA as well as next-to-leading-order QCD predictions from JETPHOX and SHERPA are compared to the measurements.
Measured cross sections for isolated-photon plus jet production as a function of $E_{\rm T}^{\gamma}$.
Measured cross sections for isolated-photon plus jet production as a function of $p_{\rm T}^{\rm jet-lead}$.
Measured cross sections for isolated-photon plus jet production as a function of $\Delta\phi^{\rm \gamma-jet\ lead}$.
The production of $W^{\pm}Z$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb$^{-1}$. The $W^{\pm}Z$ candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is $\sigma_{W^\pm Z \rightarrow \ell^{'} \nu \ell \ell}^{\textrm{fid.}} = 63.2 \pm 3.2$ (stat.) $\pm 2.6$ (sys.) $\pm 1.5$ (lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is $53.4^{+3.6}_{-2.8}$ fb. The extrapolation of the measurement from the fiducial to the total phase space yields $\sigma_{W^{\pm}Z}^{\textrm{tot.}} = 50.6 \pm 2.6$ (stat.) $\pm 2.0$ (sys.) $\pm 0.9$ (th.) $\pm 1.2$ (lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of $48.2^{+1.1}_{-1.0}$ pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent $W^+Z$ and $W^-Z$ cross sections and their ratio.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
The measured fiducial cross section in the four channels and their combination. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity uncertainty, the second is the luminosity uncertainty.
Inclusive isolated-photon production in $pp$ collisions at a centre-of-mass energy of 13 TeV is studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2 fb$^{-1}$. The cross section is measured as a function of the photon transverse energy above 125 GeV in different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $|\eta^{\gamma}|<0.6$.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $0.6<|\eta^{\gamma}|<1.37$.
Measured cross sections for inclusive isolated-photon production as a function of $E_{\rm T}^{\gamma}$ for $1.56<|\eta^{\gamma}|<1.81$.
Inclusive and differential fiducial cross sections of Higgs boson production in proton-proton collisions are measured in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel. The proton-proton collision data were produced at the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector in 2015 and 2016, corresponding to an integrated luminosity of 36.1 fb$^{-1}$. The inclusive fiducial cross section in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel is measured to be 3.62 $\pm$ 0.50 (stat) $^{+0.25}_{-0.20}$ (sys) fb, in agreement with the Standard Model prediction of 2.91 $\pm$ 0.13 fb. The cross section is also extrapolated to the total phase space including all Standard Model Higgs boson decays. Several differential fiducial cross sections are measured for observables sensitive to the Higgs boson production and decay, including kinematic distributions of jets produced in association with the Higgs boson. Good agreement is found between data and Standard Model predictions. The results are used to put constraints on anomalous Higgs boson interactions with Standard Model particles, using the pseudo-observable extension to the kappa-framework.
Measured differential fiducial cross sections in Higgs transverse momentum (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
Measured differential fiducial cross sections in Higgs rapidity (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
Measured differential fiducial cross sections in invariant mass of the subleading lepton pair (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
Measurements of fiducial and differential cross sections of Higgs boson production in the ${H \rightarrow ZZ ^{*}\rightarrow 4\ell}$ decay channel are presented. The cross sections are determined within a fiducial phase space and corrected for detection efficiency and resolution effects. They are based on 20.3 fb$^{-1}$ of $pp$ collision data, produced at $\sqrt{s}$=8 TeV centre-of-mass energy at the LHC and recorded by the ATLAS detector. The differential measurements are performed in bins of transverse momentum and rapidity of the four-lepton system, the invariant mass of the subleading lepton pair and the decay angle of the leading lepton pair with respect to the beam line in the four-lepton rest frame, as well as the number of jets and the transverse momentum of the leading jet. The measured cross sections are compared to selected theoretical calculations of the Standard Model expectations. No significant deviation from any of the tested predictions is found.
Measured differential fiducial cross sections in Higgs transverse momentum (second column). The given uncertainty includes statistical and systematic components. The third (fourth) column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ (HRes) for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fifth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.
Measured differential fiducial cross sections in the absolute value of the Higgs rapidity (second column). The given uncertainty includes statistical and systematic components. The third (fourth) column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ (HRes) for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fifth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.
Measured differential fiducial cross sections in m34, which corresponds to the invariant mass of the off-shell Z boson (second column). The given uncertainty includes statistical and systematic components. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg Minlo HJ for the ggF process, Powheg for the VBF process, and Pythia 8 for the VH and ttH process. The uncertainty includes PDF, scale, and branching fraction uncertainty. The fourth column gives the non-ggF prediction (total minus ggF). All predicted distributions were normalized to the best predicted inclusive Higgs production cross sections available at the time of the publication.
The dynamics of isolated-photon plus one-, two- and three-jet production in $pp$ collisions at a centre-of-mass energy of 8 TeV are studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 20.2 fb$^{-1}$. Measurements of isolated-photon plus jets cross sections are presented as functions of the photon and jet transverse momenta. The cross sections as functions of the azimuthal angle between the photon and the jets, the azimuthal angle between the jets, the photon-jet invariant mass and the scattering angle in the photon-jet centre-of-mass system are presented. The pattern of QCD radiation around the photon and the leading jet is investigated by measuring jet production in an annular region centred on each object; enhancements are observed around the leading jet with respect to the photon in the directions towards the beams. The experimental measurements are compared to several different theoretical calculations, and overall a good description of the data is found.
Measured cross sections for isolated-photon plus 1jet production as a function of $E_{\rm T}^{\gamma}$.
Measured cross sections for isolated-photon plus 1jet production as a function of $p_{\rm T}^{\rm jet1}$.
Measured cross sections for isolated-photon plus 1jet production as a function of $m^{\gamma-\rm jet1}$.
The production of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ charmed mesons has been measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV at the LHC, using data corresponding to an integrated luminosity of $280\,$nb$^{-1}$. The charmed mesons have been reconstructed in the range of transverse momentum $3.5<p_{\rm T}(D)<100$ GeV and pseudorapidity $|\eta(D)|<2.1$. The differential cross sections as a function of transverse momentum and pseudorapidity were measured for $D^{*\pm}$ and $D^\pm$ production. The next-to-leading-order QCD predictions are consistent with the data in the visible kinematic region within the large theoretical uncertainties. Using the visible $D$ cross sections and an extrapolation to the full kinematic phase space, the strangeness-suppression factor in charm fragmentation, the fraction of charged non-strange $D$ mesons produced in a vector state, and the total cross section of charm production at $\sqrt{s}=7$ TeV were derived.
The visible low-$p_T$, $3.5<p_T(D)<20\rm{\ GeV}$, and high-$p_T$, $20<p_T(D)<100\rm{\ GeV}$, cross sections of $D^{*\pm}$, $D^\pm$ and $D^\pm_s$ production with $|\eta|<2.1$. The data uncertainties are the total uncertainties obtained as sums in quadrature of the statistical, systematic, luminosity and branching-fraction uncertainties.
The measured differential cross sections $\rm{d}\sigma/\rm{d}p_T$ of $D^{*\pm}$ and $D^\pm$ production with $|\eta|<2.1$. The first and second errors are the statistical and systematic uncertainties, respectively. The systematic uncertainties corresponding to the tracking ($\delta_2$) uncertainties (Table 2 of the paper) are strongly correlated. The fully correlated uncertainties linked with the luminosity measurement ($3.5\%$) and branching fractions ($1.5\%$ and $2.1\%$ for $D^{*\pm}$ and $D^\pm$, respectively) are not shown.
The measured differential cross sections $\rm{d}\sigma/\rm{d}|\eta|$ of $D^{*\pm}$ and $D^\pm$ production with $3.5<p_T<20\,$GeV. The first and second errors are the statistical and systematic uncertainties, respectively. The systematic uncertainty fractions corresponding to the tracking ($\delta_2$) uncertainties (Table 2 of the paper) are strongly correlated. The fully correlated uncertainties linked with the luminosity measurement ($3.5\%$) and branching fractions ($1.5\%$ and $2.1\%$ for $D^{*\pm}$ and $D^\pm$, respectively) are not shown.
Various differential cross-sections are measured in top-quark pair ($t\bar{t}$) events produced in proton-proton collisions at a centre-of-mass energy of $\sqrt{s} = 7$ TeV at the LHC with the ATLAS detector. These differential cross-sections are presented in a data set corresponding to an integrated luminosity of $4.6$ fb$^{-1}$. The differential cross-sections are presented in terms of kinematic variables, such as momentum, rapidity and invariant mass, of a top-quark proxyreferred to as the pseudo-top-quark as well as the pseudo-top-quark pair system. The dependence of the measurement on theoretical models is minimal. The measurements are performed on $t\bar{t}$ events in the lepton+jets channel, requiring exactly one charged lepton and at least four jets with at least two of them tagged as originating from a $b$-quark. The hadronic and leptonic pseudo-top-quarks are defined via the leptonic or hadronic decay mode of the $W$ boson produced by the top-quark decay in events with a single charged lepton. Differential cross-section measurements of the pseudo-top-quark variables are compared with several Monte Carlo models that implement next-to-leading order or leading-order multi-leg matrix-element calculations.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$in the muon channel. The results shown in this table are one of the inputs for the combined results.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $p_{\mathrm{T}}(\hat{t}_{\mathrm{h}})$ in the electron channel. The results shown in this table are one of the inputs for the combined results.
Measured $t\bar{t}$ differential cross-section and relative uncertainty as a function of the hadronic pseudo-top-quark $|y(\hat{t}_{\mathrm{h}})|$ in the muon channel. The results shown in this table are one of the inputs for the combined results.
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of $\sqrt{s}=8$ TeV is presented. The results are based on an integrated luminosity of 20.2 fb$^{-1}$ recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying $|\eta^{\gamma}|<1.37$ or ${1.56<|\eta^{\gamma}|<2.37}$ and transverse energies of respectively $E_{\mathrm{T,1}}^{\gamma}>40$ GeV and $E_{\mathrm{T,2}}^{\gamma}>30$ GeV for the two leading photons ordered in transverse energy produced in the interaction.The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is $16.8 \pm 0.8$ pb. The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%.
The measured fiducial (total xs).
The measured differential as a function of Mgg.
The measured differential as a function of pTgg.
Differential cross-sections are measured for top-quark pair production in the all-hadronic decay mode, using proton$-$proton collision events collected by the ATLAS experiment in which all six decay jets are separately resolved. Absolute and normalised single- and double-differential cross-sections are measured at particle and parton level as a function of various kinematic variables. Emphasis is placed on well-measured observables in fully reconstructed final states, as well as on the study of correlations between the top-quark pair system and additional jet radiation identified in the event. The study is performed using data from proton$-$proton collisions at $\sqrt{s}=13~\mbox{TeV}$ collected by the ATLAS detector at CERN's Large Hadron Collider in 2015 and 2016, corresponding to an integrated luminosity of $\mbox{36.1 fb}^{-1}$. The rapidities of the individual top quarks and of the top-quark pair are well modelled by several independent event generators. Significant mismodelling is observed in the transverse momenta of the leading three jet emissions, while the leading top-quark transverse momentum and top-quark pair transverse momentum are both found to be incompatible with several theoretical predictions.
- - - - - - - - Overview of HEPData Record - - - - - - - - <br/><br/> <b>Fiducial phase space definition:</b><br/> <ul> <li> NLEP = 0, either E or MU, PT > 15 GeV, ABS ETA < 1.37 <li> NJETS >= 6, PT > 25 GeV, ABS ETA < 2.5 <li> NBJETS >= 2 </ul><br/> <b>Particle level:</b><br/> <u>1D:</u><br/> Spectra: <ul> <li><a href="103063?version=1&table=Table 1">1/SIG*DSIG/DDR_E1J1</a> (Table 1) <li><a href="103063?version=1&table=Table 3">DSIG/DDR_E1J1</a> (Table 3) <li><a href="103063?version=1&table=Table 5">1/SIG*DSIG/DABS_T1_Y</a> (Table 5) <li><a href="103063?version=1&table=Table 7">DSIG/DABS_T1_Y</a> (Table 7) <li><a href="103063?version=1&table=Table 9">1/SIG*DSIG/DTT_M</a> (Table 9) <li><a href="103063?version=1&table=Table 11">DSIG/DTT_M</a> (Table 11) <li><a href="103063?version=1&table=Table 13">1/SIG*DSIG/DABS_T2_Y</a> (Table 13) <li><a href="103063?version=1&table=Table 15">DSIG/DABS_T2_Y</a> (Table 15) <li><a href="103063?version=1&table=Table 17">1/SIG*DSIG/DABS_TT_Y</a> (Table 17) <li><a href="103063?version=1&table=Table 19">DSIG/DABS_TT_Y</a> (Table 19) <li><a href="103063?version=1&table=Table 21">1/SIG*DSIG/DT1_PT</a> (Table 21) <li><a href="103063?version=1&table=Table 23">DSIG/DT1_PT</a> (Table 23) <li><a href="103063?version=1&table=Table 25">1/SIG*DSIG/DT2_PT</a> (Table 25) <li><a href="103063?version=1&table=Table 27">DSIG/DT2_PT</a> (Table 27) <li><a href="103063?version=1&table=Table 29">1/SIG*DSIG/DTT_PT</a> (Table 29) <li><a href="103063?version=1&table=Table 31">DSIG/DTT_PT</a> (Table 31) <li><a href="103063?version=1&table=Table 33">1/SIG*DSIG/DN_JETS</a> (Table 33) <li><a href="103063?version=1&table=Table 35">DSIG/DN_JETS</a> (Table 35) <li><a href="103063?version=1&table=Table 37">1/SIG*DSIG/DDELTAPHI</a> (Table 37) <li><a href="103063?version=1&table=Table 39">DSIG/DDELTAPHI</a> (Table 39) <li><a href="103063?version=1&table=Table 41">1/SIG*DSIG/DABSPOUT</a> (Table 41) <li><a href="103063?version=1&table=Table 43">DSIG/DABSPOUT</a> (Table 43) <li><a href="103063?version=1&table=Table 45">1/SIG*DSIG/DABSPCROSS</a> (Table 45) <li><a href="103063?version=1&table=Table 47">DSIG/DABSPCROSS</a> (Table 47) <li><a href="103063?version=1&table=Table 49">1/SIG*DSIG/DZ_TT</a> (Table 49) <li><a href="103063?version=1&table=Table 51">DSIG/DZ_TT</a> (Table 51) <li><a href="103063?version=1&table=Table 53">1/SIG*DSIG/DHT_TT</a> (Table 53) <li><a href="103063?version=1&table=Table 55">DSIG/DHT_TT</a> (Table 55) <li><a href="103063?version=1&table=Table 57">1/SIG*DSIG/DABS_Y_BOOST </a> (Table 57) <li><a href="103063?version=1&table=Table 59">DSIG/DABS_Y_BOOST </a> (Table 59) <li><a href="103063?version=1&table=Table 61">1/SIG*DSIG/DCHI_TT</a> (Table 61) <li><a href="103063?version=1&table=Table 63">DSIG/DCHI_TT</a> (Table 63) <li><a href="103063?version=1&table=Table 65">1/SIG*DSIG/DRWT1</a> (Table 65) <li><a href="103063?version=1&table=Table 67">DSIG/DRWT1</a> (Table 67) <li><a href="103063?version=1&table=Table 69">1/SIG*DSIG/DRWT2</a> (Table 69) <li><a href="103063?version=1&table=Table 71">DSIG/DRWT2</a> (Table 71) <li><a href="103063?version=1&table=Table 73">1/SIG*DSIG/DRWB1</a> (Table 73) <li><a href="103063?version=1&table=Table 75">DSIG/DRWB1</a> (Table 75) <li><a href="103063?version=1&table=Table 77">1/SIG*DSIG/DRWB2</a> (Table 77) <li><a href="103063?version=1&table=Table 79">DSIG/DRWB2</a> (Table 79) <li><a href="103063?version=1&table=Table 81">1/SIG*DSIG/DDR_E1TC</a> (Table 81) <li><a href="103063?version=1&table=Table 83">DSIG/DDR_E1TC</a> (Table 83) <li><a href="103063?version=1&table=Table 85">1/SIG*DSIG/DDR_E2TC</a> (Table 85) <li><a href="103063?version=1&table=Table 87">DSIG/DDR_E2TC</a> (Table 87) <li><a href="103063?version=1&table=Table 89">1/SIG*DSIG/DDR_E3TC</a> (Table 89) <li><a href="103063?version=1&table=Table 91">DSIG/DDR_E3TC</a> (Table 91) <li><a href="103063?version=1&table=Table 93">1/SIG*DSIG/DRPT_E1T1</a> (Table 93) <li><a href="103063?version=1&table=Table 95">DSIG/DRPT_E1T1</a> (Table 95) <li><a href="103063?version=1&table=Table 97">1/SIG*DSIG/DRPT_E2T1</a> (Table 97) <li><a href="103063?version=1&table=Table 99">DSIG/DRPT_E2T1</a> (Table 99) <li><a href="103063?version=1&table=Table 101">1/SIG*DSIG/DRPT_E3T1</a> (Table 101) <li><a href="103063?version=1&table=Table 103">DSIG/DRPT_E3T1</a> (Table 103) <li><a href="103063?version=1&table=Table 105">1/SIG*DSIG/DRPT_TTE1</a> (Table 105) <li><a href="103063?version=1&table=Table 107">DSIG/DRPT_TTE1</a> (Table 107) <li><a href="103063?version=1&table=Table 109">1/SIG*DSIG/DRPT_E1J1</a> (Table 109) <li><a href="103063?version=1&table=Table 111">DSIG/DRPT_E1J1</a> (Table 111) <li><a href="103063?version=1&table=Table 113">1/SIG*DSIG/DRPT_E2J1</a> (Table 113) <li><a href="103063?version=1&table=Table 115">DSIG/DRPT_E2J1</a> (Table 115) <li><a href="103063?version=1&table=Table 117">1/SIG*DSIG/DRPT_E3J1</a> (Table 117) <li><a href="103063?version=1&table=Table 119">DSIG/DRPT_E3J1</a> (Table 119) <li><a href="103063?version=1&table=Table 121">1/SIG*DSIG/DDR_E2E1</a> (Table 121) <li><a href="103063?version=1&table=Table 123">DSIG/DDR_E2E1</a> (Table 123) <li><a href="103063?version=1&table=Table 125">1/SIG*DSIG/DDR_E3E1</a> (Table 125) <li><a href="103063?version=1&table=Table 127">DSIG/DDR_E3E1</a> (Table 127) <li><a href="103063?version=1&table=Table 129">1/SIG*DSIG/DRPT_E2E1</a> (Table 129) <li><a href="103063?version=1&table=Table 131">DSIG/DRPT_E2E1</a> (Table 131) <li><a href="103063?version=1&table=Table 133">1/SIG*DSIG/DRPT_E3E1</a> (Table 133) <li><a href="103063?version=1&table=Table 135">DSIG/DRPT_E3E1</a> (Table 135) <li><a href="103063?version=1&table=Table 137">SIG</a> (Table 137) </ul><br/> Covariances: <ul> <li><a href="103063?version=1&table=Table 2">1/SIG*DSIG/DDR_E1J1</a> (Table 2) <li><a href="103063?version=1&table=Table 4">DSIG/DDR_E1J1</a> (Table 4) <li><a href="103063?version=1&table=Table 6">1/SIG*DSIG/DABS_T1_Y</a> (Table 6) <li><a href="103063?version=1&table=Table 8">DSIG/DABS_T1_Y</a> (Table 8) <li><a href="103063?version=1&table=Table 10">1/SIG*DSIG/DTT_M</a> (Table 10) <li><a href="103063?version=1&table=Table 12">DSIG/DTT_M</a> (Table 12) <li><a href="103063?version=1&table=Table 14">1/SIG*DSIG/DABS_T2_Y</a> (Table 14) <li><a href="103063?version=1&table=Table 16">DSIG/DABS_T2_Y</a> (Table 16) <li><a href="103063?version=1&table=Table 18">1/SIG*DSIG/DABS_TT_Y</a> (Table 18) <li><a href="103063?version=1&table=Table 20">DSIG/DABS_TT_Y</a> (Table 20) <li><a href="103063?version=1&table=Table 22">1/SIG*DSIG/DT1_PT</a> (Table 22) <li><a href="103063?version=1&table=Table 24">DSIG/DT1_PT</a> (Table 24) <li><a href="103063?version=1&table=Table 26">1/SIG*DSIG/DT2_PT</a> (Table 26) <li><a href="103063?version=1&table=Table 28">DSIG/DT2_PT</a> (Table 28) <li><a href="103063?version=1&table=Table 30">1/SIG*DSIG/DTT_PT</a> (Table 30) <li><a href="103063?version=1&table=Table 32">DSIG/DTT_PT</a> (Table 32) <li><a href="103063?version=1&table=Table 34">1/SIG*DSIG/DN_JETS</a> (Table 34) <li><a href="103063?version=1&table=Table 36">DSIG/DN_JETS</a> (Table 36) <li><a href="103063?version=1&table=Table 38">1/SIG*DSIG/DDELTAPHI</a> (Table 38) <li><a href="103063?version=1&table=Table 40">DSIG/DDELTAPHI</a> (Table 40) <li><a href="103063?version=1&table=Table 42">1/SIG*DSIG/DABSPOUT</a> (Table 42) <li><a href="103063?version=1&table=Table 44">DSIG/DABSPOUT</a> (Table 44) <li><a href="103063?version=1&table=Table 46">1/SIG*DSIG/DABSPCROSS</a> (Table 46) <li><a href="103063?version=1&table=Table 48">DSIG/DABSPCROSS</a> (Table 48) <li><a href="103063?version=1&table=Table 50">1/SIG*DSIG/DZ_TT</a> (Table 50) <li><a href="103063?version=1&table=Table 52">DSIG/DZ_TT</a> (Table 52) <li><a href="103063?version=1&table=Table 54">1/SIG*DSIG/DHT_TT</a> (Table 54) <li><a href="103063?version=1&table=Table 56">DSIG/DHT_TT</a> (Table 56) <li><a href="103063?version=1&table=Table 58">1/SIG*DSIG/DABS_Y_BOOST </a> (Table 58) <li><a href="103063?version=1&table=Table 60">DSIG/DABS_Y_BOOST </a> (Table 60) <li><a href="103063?version=1&table=Table 62">1/SIG*DSIG/DCHI_TT</a> (Table 62) <li><a href="103063?version=1&table=Table 64">DSIG/DCHI_TT</a> (Table 64) <li><a href="103063?version=1&table=Table 66">1/SIG*DSIG/DRWT1</a> (Table 66) <li><a href="103063?version=1&table=Table 68">DSIG/DRWT1</a> (Table 68) <li><a href="103063?version=1&table=Table 70">1/SIG*DSIG/DRWT2</a> (Table 70) <li><a href="103063?version=1&table=Table 72">DSIG/DRWT2</a> (Table 72) <li><a href="103063?version=1&table=Table 74">1/SIG*DSIG/DRWB1</a> (Table 74) <li><a href="103063?version=1&table=Table 76">DSIG/DRWB1</a> (Table 76) <li><a href="103063?version=1&table=Table 78">1/SIG*DSIG/DRWB2</a> (Table 78) <li><a href="103063?version=1&table=Table 80">DSIG/DRWB2</a> (Table 80) <li><a href="103063?version=1&table=Table 82">1/SIG*DSIG/DDR_E1TC</a> (Table 82) <li><a href="103063?version=1&table=Table 84">DSIG/DDR_E1TC</a> (Table 84) <li><a href="103063?version=1&table=Table 86">1/SIG*DSIG/DDR_E2TC</a> (Table 86) <li><a href="103063?version=1&table=Table 88">DSIG/DDR_E2TC</a> (Table 88) <li><a href="103063?version=1&table=Table 90">1/SIG*DSIG/DDR_E3TC</a> (Table 90) <li><a href="103063?version=1&table=Table 92">DSIG/DDR_E3TC</a> (Table 92) <li><a href="103063?version=1&table=Table 94">1/SIG*DSIG/DRPT_E1T1</a> (Table 94) <li><a href="103063?version=1&table=Table 96">DSIG/DRPT_E1T1</a> (Table 96) <li><a href="103063?version=1&table=Table 98">1/SIG*DSIG/DRPT_E2T1</a> (Table 98) <li><a href="103063?version=1&table=Table 100">DSIG/DRPT_E2T1</a> (Table 100) <li><a href="103063?version=1&table=Table 102">1/SIG*DSIG/DRPT_E3T1</a> (Table 102) <li><a href="103063?version=1&table=Table 104">DSIG/DRPT_E3T1</a> (Table 104) <li><a href="103063?version=1&table=Table 106">1/SIG*DSIG/DRPT_TTE1</a> (Table 106) <li><a href="103063?version=1&table=Table 108">DSIG/DRPT_TTE1</a> (Table 108) <li><a href="103063?version=1&table=Table 110">1/SIG*DSIG/DRPT_E1J1</a> (Table 110) <li><a href="103063?version=1&table=Table 112">DSIG/DRPT_E1J1</a> (Table 112) <li><a href="103063?version=1&table=Table 114">1/SIG*DSIG/DRPT_E2J1</a> (Table 114) <li><a href="103063?version=1&table=Table 116">DSIG/DRPT_E2J1</a> (Table 116) <li><a href="103063?version=1&table=Table 118">1/SIG*DSIG/DRPT_E3J1</a> (Table 118) <li><a href="103063?version=1&table=Table 120">DSIG/DRPT_E3J1</a> (Table 120) <li><a href="103063?version=1&table=Table 122">1/SIG*DSIG/DDR_E2E1</a> (Table 122) <li><a href="103063?version=1&table=Table 124">DSIG/DDR_E2E1</a> (Table 124) <li><a href="103063?version=1&table=Table 126">1/SIG*DSIG/DDR_E3E1</a> (Table 126) <li><a href="103063?version=1&table=Table 128">DSIG/DDR_E3E1</a> (Table 128) <li><a href="103063?version=1&table=Table 130">1/SIG*DSIG/DRPT_E2E1</a> (Table 130) <li><a href="103063?version=1&table=Table 132">DSIG/DRPT_E2E1</a> (Table 132) <li><a href="103063?version=1&table=Table 134">1/SIG*DSIG/DRPT_E3E1</a> (Table 134) <li><a href="103063?version=1&table=Table 136">DSIG/DRPT_E3E1</a> (Table 136) </ul><br/> <u>2D:</u><br/> Spectra: <ul> <li><a href="103063?version=1&table=Table 138">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 6)</a> (Table 138) <li><a href="103063?version=1&table=Table 139">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 7)</a> (Table 139) <li><a href="103063?version=1&table=Table 140">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS = 8)</a> (Table 140) <li><a href="103063?version=1&table=Table 141">1/SIG*D2SIG/DT1_PT/DN_JETS (N_JETS > 8)</a> (Table 141) <li><a href="103063?version=1&table=Table 152">D2SIG/DT1_PT/DN_JETS (N_JETS = 6)</a> (Table 152) <li><a href="103063?version=1&table=Table 153">D2SIG/DT1_PT/DN_JETS (N_JETS = 7)</a> (Table 153) <li><a href="103063?version=1&table=Table 154">D2SIG/DT1_PT/DN_JETS (N_JETS = 8)</a> (Table 154) <li><a href="103063?version=1&table=Table 155">D2SIG/DT1_PT/DN_JETS (N_JETS > 8)</a> (Table 155) <li><a href="103063?version=1&table=Table 166">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 6)</a> (Table 166) <li><a href="103063?version=1&table=Table 167">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 7)</a> (Table 167) <li><a href="103063?version=1&table=Table 168">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS = 8)</a> (Table 168) <li><a href="103063?version=1&table=Table 169">1/SIG*D2SIG/DT2_PT/DN_JETS (N_JETS > 8)</a> (Table 169) <li><a href="103063?version=1&table=Table 180">D2SIG/DT2_PT/DN_JETS (N_JETS = 6)</a> (Table 180) <li><a href="103063?version=1&table=Table 181">D2SIG/DT2_PT/DN_JETS (N_JETS = 7)</a> (Table 181) <li><a href="103063?version=1&table=Table 182">D2SIG/DT2_PT/DN_JETS (N_JETS = 8)</a> (Table 182) <li><a href="103063?version=1&table=Table 183">D2SIG/DT2_PT/DN_JETS (N_JETS > 8)</a> (Table 183) <li><a href="103063?version=1&table=Table 194">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 6)</a> (Table 194) <li><a href="103063?version=1&table=Table 195">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 7)</a> (Table 195) <li><a href="103063?version=1&table=Table 196">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS = 8)</a> (Table 196) <li><a href="103063?version=1&table=Table 197">1/SIG*D2SIG/DTT_PT/DN_JETS (N_JETS > 8)</a> (Table 197) <li><a href="103063?version=1&table=Table 208">D2SIG/DTT_PT/DN_JETS (N_JETS = 6)</a> (Table 208) <li><a href="103063?version=1&table=Table 209">D2SIG/DTT_PT/DN_JETS (N_JETS = 7)</a> (Table 209) <li><a href="103063?version=1&table=Table 210">D2SIG/DTT_PT/DN_JETS (N_JETS = 8)</a> (Table 210) <li><a href="103063?version=1&table=Table 211">D2SIG/DTT_PT/DN_JETS (N_JETS > 8)</a> (Table 211) <li><a href="103063?version=1&table=Table 222">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 6)</a> (Table 222) <li><a href="103063?version=1&table=Table 223">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 7)</a> (Table 223) <li><a href="103063?version=1&table=Table 224">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS = 8)</a> (Table 224) <li><a href="103063?version=1&table=Table 225">1/SIG*D2SIG/DABSPOUT/DN_JETS (N_JETS > 8)</a> (Table 225) <li><a href="103063?version=1&table=Table 236">D2SIG/DABSPOUT/DN_JETS (N_JETS = 6)</a> (Table 236) <li><a href="103063?version=1&table=Table 237">D2SIG/DABSPOUT/DN_JETS (N_JETS = 7)</a> (Table 237) <li><a href="103063?version=1&table=Table 238">D2SIG/DABSPOUT/DN_JETS (N_JETS = 8)</a> (Table 238) <li><a href="103063?version=1&table=Table 239">D2SIG/DABSPOUT/DN_JETS (N_JETS > 8)</a> (Table 239) <li><a href="103063?version=1&table=Table 250">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 6)</a> (Table 250) <li><a href="103063?version=1&table=Table 251">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 7)</a> (Table 251) <li><a href="103063?version=1&table=Table 252">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS = 8)</a> (Table 252) <li><a href="103063?version=1&table=Table 253">1/SIG*D2SIG/DDELTAPHI/DN_JETS (N_JETS > 8)</a> (Table 253) <li><a href="103063?version=1&table=Table 264">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 6)</a> (Table 264) <li><a href="103063?version=1&table=Table 265">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 7)</a> (Table 265) <li><a href="103063?version=1&table=Table 266">D2SIG/DDELTAPHI/DN_JETS (N_JETS = 8)</a> (Table 266) <li><a href="103063?version=1&table=Table 267">D2SIG/DDELTAPHI/DN_JETS (N_JETS > 8)</a> (Table 267) <li><a href="103063?version=1&table=Table 278">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 6)</a> (Table 278) <li><a href="103063?version=1&table=Table 279">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 7)</a> (Table 279) <li><a href="103063?version=1&table=Table 280">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS = 8)</a> (Table 280) <li><a href="103063?version=1&table=Table 281">1/SIG*D2SIG/DABSPCROSS/DN_JETS (N_JETS > 8)</a> (Table 281) <li><a href="103063?version=1&table=Table 292">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 6)</a> (Table 292) <li><a href="103063?version=1&table=Table 293">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 7)</a> (Table 293) <li><a href="103063?version=1&table=Table 294">D2SIG/DABSPCROSS/DN_JETS (N_JETS = 8)</a> (Table 294) <li><a href="103063?version=1&table=Table 295">D2SIG/DABSPCROSS/DN_JETS (N_JETS > 8)</a> (Table 295) <li><a href="103063?version=1&table=Table 306">1/SIG*D2SIG/DT2_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 306) <li><a href="103063?version=1&table=Table 307">1/SIG*D2SIG/DT2_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 307) <li><a href="103063?version=1&table=Table 308">1/SIG*D2SIG/DT2_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 308) <li><a href="103063?version=1&table=Table 309">1/SIG*D2SIG/DT2_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 309) <li><a href="103063?version=1&table=Table 320">D2SIG/DT2_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 320) <li><a href="103063?version=1&table=Table 321">D2SIG/DT2_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 321) <li><a href="103063?version=1&table=Table 322">D2SIG/DT2_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 322) <li><a href="103063?version=1&table=Table 323">D2SIG/DT2_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 323) <li><a href="103063?version=1&table=Table 334">1/SIG*D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 334) <li><a href="103063?version=1&table=Table 335">1/SIG*D2SIG/DTT_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 335) <li><a href="103063?version=1&table=Table 336">1/SIG*D2SIG/DTT_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 336) <li><a href="103063?version=1&table=Table 337">1/SIG*D2SIG/DTT_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 337) <li><a href="103063?version=1&table=Table 348">D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 348) <li><a href="103063?version=1&table=Table 349">D2SIG/DTT_PT/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 349) <li><a href="103063?version=1&table=Table 350">D2SIG/DTT_PT/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 350) <li><a href="103063?version=1&table=Table 351">D2SIG/DTT_PT/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 351) <li><a href="103063?version=1&table=Table 362">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 362) <li><a href="103063?version=1&table=Table 363">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 363) <li><a href="103063?version=1&table=Table 364">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 364) <li><a href="103063?version=1&table=Table 365">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 365) <li><a href="103063?version=1&table=Table 376">D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 620.0 GeV)</a> (Table 376) <li><a href="103063?version=1&table=Table 377">D2SIG/DABS_TT_Y/DTT_M ( 620.0 GeV < TT_M < 835.0 GeV)</a> (Table 377) <li><a href="103063?version=1&table=Table 378">D2SIG/DABS_TT_Y/DTT_M ( 835.0 GeV < TT_M < 1050.0 GeV)</a> (Table 378) <li><a href="103063?version=1&table=Table 379">D2SIG/DABS_TT_Y/DTT_M ( 1050.0 GeV < TT_M < 3000.0 GeV)</a> (Table 379) <li><a href="103063?version=1&table=Table 390">1/SIG*D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 175.0 GeV)</a> (Table 390) <li><a href="103063?version=1&table=Table 391">1/SIG*D2SIG/DT1_PT/DT2_PT ( 175.0 GeV < T2_PT < 275.0 GeV)</a> (Table 391) <li><a href="103063?version=1&table=Table 392">1/SIG*D2SIG/DT1_PT/DT2_PT ( 275.0 GeV < T2_PT < 385.0 GeV)</a> (Table 392) <li><a href="103063?version=1&table=Table 393">1/SIG*D2SIG/DT1_PT/DT2_PT ( 385.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 393) <li><a href="103063?version=1&table=Table 404">D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 175.0 GeV)</a> (Table 404) <li><a href="103063?version=1&table=Table 405">D2SIG/DT1_PT/DT2_PT ( 175.0 GeV < T2_PT < 275.0 GeV)</a> (Table 405) <li><a href="103063?version=1&table=Table 406">D2SIG/DT1_PT/DT2_PT ( 275.0 GeV < T2_PT < 385.0 GeV)</a> (Table 406) <li><a href="103063?version=1&table=Table 407">D2SIG/DT1_PT/DT2_PT ( 385.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 407) <li><a href="103063?version=1&table=Table 418">1/SIG*D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 645.0 GeV)</a> (Table 418) <li><a href="103063?version=1&table=Table 419">1/SIG*D2SIG/DT1_PT/DTT_M ( 645.0 GeV < TT_M < 795.0 GeV)</a> (Table 419) <li><a href="103063?version=1&table=Table 420">1/SIG*D2SIG/DT1_PT/DTT_M ( 795.0 GeV < TT_M < 1080.0 GeV)</a> (Table 420) <li><a href="103063?version=1&table=Table 421">1/SIG*D2SIG/DT1_PT/DTT_M ( 1080.0 GeV < TT_M < 3000.0 GeV)</a> (Table 421) <li><a href="103063?version=1&table=Table 432">D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 645.0 GeV)</a> (Table 432) <li><a href="103063?version=1&table=Table 433">D2SIG/DT1_PT/DTT_M ( 645.0 GeV < TT_M < 795.0 GeV)</a> (Table 433) <li><a href="103063?version=1&table=Table 434">D2SIG/DT1_PT/DTT_M ( 795.0 GeV < TT_M < 1080.0 GeV)</a> (Table 434) <li><a href="103063?version=1&table=Table 435">D2SIG/DT1_PT/DTT_M ( 1080.0 GeV < TT_M < 3000.0 GeV)</a> (Table 435) </ul><br/> Covariances:<br/><ul> <li><a href="103063?version=1&table=Table 142">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 142) <li><a href="103063?version=1&table=Table 143">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 143) <li><a href="103063?version=1&table=Table 144">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 144) <li><a href="103063?version=1&table=Table 145">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 145) <li><a href="103063?version=1&table=Table 146">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 146) <li><a href="103063?version=1&table=Table 147">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 147) <li><a href="103063?version=1&table=Table 148">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 148) <li><a href="103063?version=1&table=Table 149">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 149) <li><a href="103063?version=1&table=Table 150">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 150) <li><a href="103063?version=1&table=Table 151">Matrix for 1/SIG*D2SIG/DT1_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 151) <li><a href="103063?version=1&table=Table 156">Matrix for D2SIG/DT1_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 156) <li><a href="103063?version=1&table=Table 157">Matrix for D2SIG/DT1_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 157) <li><a href="103063?version=1&table=Table 158">Matrix for D2SIG/DT1_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 158) <li><a href="103063?version=1&table=Table 159">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 159) <li><a href="103063?version=1&table=Table 160">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 160) <li><a href="103063?version=1&table=Table 161">Matrix for D2SIG/DT1_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 161) <li><a href="103063?version=1&table=Table 162">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 162) <li><a href="103063?version=1&table=Table 163">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 163) <li><a href="103063?version=1&table=Table 164">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 164) <li><a href="103063?version=1&table=Table 165">Matrix for D2SIG/DT1_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 165) <li><a href="103063?version=1&table=Table 170">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 170) <li><a href="103063?version=1&table=Table 171">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 171) <li><a href="103063?version=1&table=Table 172">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 172) <li><a href="103063?version=1&table=Table 173">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 173) <li><a href="103063?version=1&table=Table 174">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 174) <li><a href="103063?version=1&table=Table 175">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 175) <li><a href="103063?version=1&table=Table 176">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 176) <li><a href="103063?version=1&table=Table 177">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 177) <li><a href="103063?version=1&table=Table 178">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 178) <li><a href="103063?version=1&table=Table 179">Matrix for 1/SIG*D2SIG/DT2_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 179) <li><a href="103063?version=1&table=Table 184">Matrix for D2SIG/DT2_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 184) <li><a href="103063?version=1&table=Table 185">Matrix for D2SIG/DT2_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 185) <li><a href="103063?version=1&table=Table 186">Matrix for D2SIG/DT2_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 186) <li><a href="103063?version=1&table=Table 187">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 187) <li><a href="103063?version=1&table=Table 188">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 188) <li><a href="103063?version=1&table=Table 189">Matrix for D2SIG/DT2_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 189) <li><a href="103063?version=1&table=Table 190">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 190) <li><a href="103063?version=1&table=Table 191">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 191) <li><a href="103063?version=1&table=Table 192">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 192) <li><a href="103063?version=1&table=Table 193">Matrix for D2SIG/DT2_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 193) <li><a href="103063?version=1&table=Table 198">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 198) <li><a href="103063?version=1&table=Table 199">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 199) <li><a href="103063?version=1&table=Table 200">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 200) <li><a href="103063?version=1&table=Table 201">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 201) <li><a href="103063?version=1&table=Table 202">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 202) <li><a href="103063?version=1&table=Table 203">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 203) <li><a href="103063?version=1&table=Table 204">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 204) <li><a href="103063?version=1&table=Table 205">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 205) <li><a href="103063?version=1&table=Table 206">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 206) <li><a href="103063?version=1&table=Table 207">Matrix for 1/SIG*D2SIG/DTT_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 207) <li><a href="103063?version=1&table=Table 212">Matrix for D2SIG/DTT_PT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 212) <li><a href="103063?version=1&table=Table 213">Matrix for D2SIG/DTT_PT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 213) <li><a href="103063?version=1&table=Table 214">Matrix for D2SIG/DTT_PT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 214) <li><a href="103063?version=1&table=Table 215">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 215) <li><a href="103063?version=1&table=Table 216">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 216) <li><a href="103063?version=1&table=Table 217">Matrix for D2SIG/DTT_PT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 217) <li><a href="103063?version=1&table=Table 218">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 218) <li><a href="103063?version=1&table=Table 219">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 219) <li><a href="103063?version=1&table=Table 220">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 220) <li><a href="103063?version=1&table=Table 221">Matrix for D2SIG/DTT_PT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 221) <li><a href="103063?version=1&table=Table 226">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 226) <li><a href="103063?version=1&table=Table 227">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 227) <li><a href="103063?version=1&table=Table 228">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 228) <li><a href="103063?version=1&table=Table 229">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 229) <li><a href="103063?version=1&table=Table 230">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 230) <li><a href="103063?version=1&table=Table 231">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 231) <li><a href="103063?version=1&table=Table 232">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 232) <li><a href="103063?version=1&table=Table 233">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 233) <li><a href="103063?version=1&table=Table 234">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 234) <li><a href="103063?version=1&table=Table 235">Matrix for 1/SIG*D2SIG/DABSPOUT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 235) <li><a href="103063?version=1&table=Table 240">Matrix for D2SIG/DABSPOUT/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 240) <li><a href="103063?version=1&table=Table 241">Matrix for D2SIG/DABSPOUT/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 241) <li><a href="103063?version=1&table=Table 242">Matrix for D2SIG/DABSPOUT/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 242) <li><a href="103063?version=1&table=Table 243">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 243) <li><a href="103063?version=1&table=Table 244">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 244) <li><a href="103063?version=1&table=Table 245">Matrix for D2SIG/DABSPOUT/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 245) <li><a href="103063?version=1&table=Table 246">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 246) <li><a href="103063?version=1&table=Table 247">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 247) <li><a href="103063?version=1&table=Table 248">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 248) <li><a href="103063?version=1&table=Table 249">Matrix for D2SIG/DABSPOUT/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 249) <li><a href="103063?version=1&table=Table 254">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 254) <li><a href="103063?version=1&table=Table 255">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 255) <li><a href="103063?version=1&table=Table 256">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 256) <li><a href="103063?version=1&table=Table 257">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 257) <li><a href="103063?version=1&table=Table 258">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 258) <li><a href="103063?version=1&table=Table 259">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 259) <li><a href="103063?version=1&table=Table 260">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 260) <li><a href="103063?version=1&table=Table 261">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 261) <li><a href="103063?version=1&table=Table 262">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 262) <li><a href="103063?version=1&table=Table 263">Matrix for 1/SIG*D2SIG/DDELTAPHI/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 263) <li><a href="103063?version=1&table=Table 268">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 268) <li><a href="103063?version=1&table=Table 269">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 269) <li><a href="103063?version=1&table=Table 270">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 270) <li><a href="103063?version=1&table=Table 271">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 271) <li><a href="103063?version=1&table=Table 272">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 272) <li><a href="103063?version=1&table=Table 273">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 273) <li><a href="103063?version=1&table=Table 274">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 274) <li><a href="103063?version=1&table=Table 275">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 275) <li><a href="103063?version=1&table=Table 276">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 276) <li><a href="103063?version=1&table=Table 277">Matrix for D2SIG/DDELTAPHI/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 277) <li><a href="103063?version=1&table=Table 282">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 282) <li><a href="103063?version=1&table=Table 283">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 283) <li><a href="103063?version=1&table=Table 284">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 284) <li><a href="103063?version=1&table=Table 285">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 285) <li><a href="103063?version=1&table=Table 286">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 286) <li><a href="103063?version=1&table=Table 287">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 287) <li><a href="103063?version=1&table=Table 288">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 288) <li><a href="103063?version=1&table=Table 289">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 289) <li><a href="103063?version=1&table=Table 290">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 290) <li><a href="103063?version=1&table=Table 291">Matrix for 1/SIG*D2SIG/DABSPCROSS/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 291) <li><a href="103063?version=1&table=Table 296">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 1th and 1th bins of N_JETS</a> (Table 296) <li><a href="103063?version=1&table=Table 297">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 2th and 1th bins of N_JETS</a> (Table 297) <li><a href="103063?version=1&table=Table 298">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 2th and 2th bins of N_JETS</a> (Table 298) <li><a href="103063?version=1&table=Table 299">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 1th bins of N_JETS</a> (Table 299) <li><a href="103063?version=1&table=Table 300">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 2th bins of N_JETS</a> (Table 300) <li><a href="103063?version=1&table=Table 301">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 3th and 3th bins of N_JETS</a> (Table 301) <li><a href="103063?version=1&table=Table 302">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 1th bins of N_JETS</a> (Table 302) <li><a href="103063?version=1&table=Table 303">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 2th bins of N_JETS</a> (Table 303) <li><a href="103063?version=1&table=Table 304">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 3th bins of N_JETS</a> (Table 304) <li><a href="103063?version=1&table=Table 305">Matrix for D2SIG/DABSPCROSS/DN_JETS between the 4th and 4th bins of N_JETS</a> (Table 305) <li><a href="103063?version=1&table=Table 310">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 310) <li><a href="103063?version=1&table=Table 311">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 311) <li><a href="103063?version=1&table=Table 312">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 312) <li><a href="103063?version=1&table=Table 313">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 313) <li><a href="103063?version=1&table=Table 314">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 314) <li><a href="103063?version=1&table=Table 315">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 315) <li><a href="103063?version=1&table=Table 316">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 316) <li><a href="103063?version=1&table=Table 317">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 317) <li><a href="103063?version=1&table=Table 318">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 318) <li><a href="103063?version=1&table=Table 319">Matrix for 1/SIG*D2SIG/DT2_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 319) <li><a href="103063?version=1&table=Table 324">Matrix for D2SIG/DT2_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 324) <li><a href="103063?version=1&table=Table 325">Matrix for D2SIG/DT2_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 325) <li><a href="103063?version=1&table=Table 326">Matrix for D2SIG/DT2_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 326) <li><a href="103063?version=1&table=Table 327">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 327) <li><a href="103063?version=1&table=Table 328">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 328) <li><a href="103063?version=1&table=Table 329">Matrix for D2SIG/DT2_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 329) <li><a href="103063?version=1&table=Table 330">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 330) <li><a href="103063?version=1&table=Table 331">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 331) <li><a href="103063?version=1&table=Table 332">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 332) <li><a href="103063?version=1&table=Table 333">Matrix for D2SIG/DT2_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 333) <li><a href="103063?version=1&table=Table 338">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 338) <li><a href="103063?version=1&table=Table 339">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 339) <li><a href="103063?version=1&table=Table 340">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 340) <li><a href="103063?version=1&table=Table 341">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 341) <li><a href="103063?version=1&table=Table 342">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 342) <li><a href="103063?version=1&table=Table 343">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 343) <li><a href="103063?version=1&table=Table 344">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 344) <li><a href="103063?version=1&table=Table 345">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 345) <li><a href="103063?version=1&table=Table 346">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 346) <li><a href="103063?version=1&table=Table 347">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 347) <li><a href="103063?version=1&table=Table 352">Matrix for D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 352) <li><a href="103063?version=1&table=Table 353">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 353) <li><a href="103063?version=1&table=Table 354">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 354) <li><a href="103063?version=1&table=Table 355">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 355) <li><a href="103063?version=1&table=Table 356">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 356) <li><a href="103063?version=1&table=Table 357">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 357) <li><a href="103063?version=1&table=Table 358">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 358) <li><a href="103063?version=1&table=Table 359">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 359) <li><a href="103063?version=1&table=Table 360">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 360) <li><a href="103063?version=1&table=Table 361">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 361) <li><a href="103063?version=1&table=Table 366">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 366) <li><a href="103063?version=1&table=Table 367">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 367) <li><a href="103063?version=1&table=Table 368">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 368) <li><a href="103063?version=1&table=Table 369">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 369) <li><a href="103063?version=1&table=Table 370">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 370) <li><a href="103063?version=1&table=Table 371">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 371) <li><a href="103063?version=1&table=Table 372">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 1th bins of TT_M</a> (Table 372) <li><a href="103063?version=1&table=Table 373">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 2th bins of TT_M</a> (Table 373) <li><a href="103063?version=1&table=Table 374">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 3th bins of TT_M</a> (Table 374) <li><a href="103063?version=1&table=Table 375">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 4th and 4th bins of TT_M</a> (Table 375) <li><a href="103063?version=1&table=Table 380">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 380) <li><a href="103063?version=1&table=Table 381">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 381) <li><a href="103063?version=1&table=Table 382">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 382) <li><a href="103063?version=1&table=Table 383">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 383) <li><a href="103063?version=1&table=Table 384">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 384) <li><a href="103063?version=1&table=Table 385">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 385) <li><a href="103063?version=1&table=Table 386">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 1th bins of TT_M</a> (Table 386) <li><a href="103063?version=1&table=Table 387">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 2th bins of TT_M</a> (Table 387) <li><a href="103063?version=1&table=Table 388">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 3th bins of TT_M</a> (Table 388) <li><a href="103063?version=1&table=Table 389">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 4th and 4th bins of TT_M</a> (Table 389) <li><a href="103063?version=1&table=Table 394">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 394) <li><a href="103063?version=1&table=Table 395">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 395) <li><a href="103063?version=1&table=Table 396">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 396) <li><a href="103063?version=1&table=Table 397">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 397) <li><a href="103063?version=1&table=Table 398">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 398) <li><a href="103063?version=1&table=Table 399">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 399) <li><a href="103063?version=1&table=Table 400">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 400) <li><a href="103063?version=1&table=Table 401">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 401) <li><a href="103063?version=1&table=Table 402">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 402) <li><a href="103063?version=1&table=Table 403">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 403) <li><a href="103063?version=1&table=Table 408">Matrix for D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 408) <li><a href="103063?version=1&table=Table 409">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 409) <li><a href="103063?version=1&table=Table 410">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 410) <li><a href="103063?version=1&table=Table 411">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 411) <li><a href="103063?version=1&table=Table 412">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 412) <li><a href="103063?version=1&table=Table 413">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 413) <li><a href="103063?version=1&table=Table 414">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 414) <li><a href="103063?version=1&table=Table 415">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 415) <li><a href="103063?version=1&table=Table 416">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 416) <li><a href="103063?version=1&table=Table 417">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 417) <li><a href="103063?version=1&table=Table 422">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 422) <li><a href="103063?version=1&table=Table 423">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 423) <li><a href="103063?version=1&table=Table 424">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 424) <li><a href="103063?version=1&table=Table 425">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 425) <li><a href="103063?version=1&table=Table 426">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 426) <li><a href="103063?version=1&table=Table 427">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 427) <li><a href="103063?version=1&table=Table 428">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 428) <li><a href="103063?version=1&table=Table 429">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 429) <li><a href="103063?version=1&table=Table 430">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 430) <li><a href="103063?version=1&table=Table 431">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 431) <li><a href="103063?version=1&table=Table 436">Matrix for D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 436) <li><a href="103063?version=1&table=Table 437">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 437) <li><a href="103063?version=1&table=Table 438">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 438) <li><a href="103063?version=1&table=Table 439">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 439) <li><a href="103063?version=1&table=Table 440">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 440) <li><a href="103063?version=1&table=Table 441">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 441) <li><a href="103063?version=1&table=Table 442">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 442) <li><a href="103063?version=1&table=Table 443">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 443) <li><a href="103063?version=1&table=Table 444">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 444) <li><a href="103063?version=1&table=Table 445">Matrix for D2SIG/DT1_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 445) </ul><br/> <b>Parton level:</b><br/> <u>1D:</u><br/> Spectra:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 446">1/SIG*DSIG/DCHI_TT</a> (Table 446) <li><a href="103063?version=1&table=Table 448">DSIG/DCHI_TT</a> (Table 448) <li><a href="103063?version=1&table=Table 450">1/SIG*DSIG/DTT_PT</a> (Table 450) <li><a href="103063?version=1&table=Table 452">DSIG/DTT_PT</a> (Table 452) <li><a href="103063?version=1&table=Table 454">1/SIG*DSIG/DDELTAPHI</a> (Table 454) <li><a href="103063?version=1&table=Table 456">DSIG/DDELTAPHI</a> (Table 456) <li><a href="103063?version=1&table=Table 458">1/SIG*DSIG/DT2_PT</a> (Table 458) <li><a href="103063?version=1&table=Table 460">DSIG/DT2_PT</a> (Table 460) <li><a href="103063?version=1&table=Table 462">1/SIG*DSIG/DTT_M</a> (Table 462) <li><a href="103063?version=1&table=Table 464">DSIG/DTT_M</a> (Table 464) <li><a href="103063?version=1&table=Table 466">1/SIG*DSIG/DABS_Y_BOOST</a> (Table 466) <li><a href="103063?version=1&table=Table 468">DSIG/DABS_Y_BOOST</a> (Table 468) <li><a href="103063?version=1&table=Table 470">1/SIG*DSIG/DT1_PT</a> (Table 470) <li><a href="103063?version=1&table=Table 472">DSIG/DT1_PT</a> (Table 472) <li><a href="103063?version=1&table=Table 474">1/SIG*DSIG/DABS_TT_Y</a> (Table 474) <li><a href="103063?version=1&table=Table 476">DSIG/DABS_TT_Y</a> (Table 476) <li><a href="103063?version=1&table=Table 478">1/SIG*DSIG/DABS_T2_Y</a> (Table 478) <li><a href="103063?version=1&table=Table 480">DSIG/DABS_T2_Y</a> (Table 480) <li><a href="103063?version=1&table=Table 482">1/SIG*DSIG/DHT_TT</a> (Table 482) <li><a href="103063?version=1&table=Table 484">DSIG/DHT_TT</a> (Table 484) <li><a href="103063?version=1&table=Table 486">1/SIG*DSIG/DABS_T1_Y</a> (Table 486) <li><a href="103063?version=1&table=Table 488">DSIG/DABS_T1_Y</a> (Table 488) </ul><br/> Covariances:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 447">1/SIG*DSIG/DCHI_TT</a> (Table 447) <li><a href="103063?version=1&table=Table 449">DSIG/DCHI_TT</a> (Table 449) <li><a href="103063?version=1&table=Table 451">1/SIG*DSIG/DTT_PT</a> (Table 451) <li><a href="103063?version=1&table=Table 453">DSIG/DTT_PT</a> (Table 453) <li><a href="103063?version=1&table=Table 455">1/SIG*DSIG/DDELTAPHI</a> (Table 455) <li><a href="103063?version=1&table=Table 457">DSIG/DDELTAPHI</a> (Table 457) <li><a href="103063?version=1&table=Table 459">1/SIG*DSIG/DT2_PT</a> (Table 459) <li><a href="103063?version=1&table=Table 461">DSIG/DT2_PT</a> (Table 461) <li><a href="103063?version=1&table=Table 463">1/SIG*DSIG/DTT_M</a> (Table 463) <li><a href="103063?version=1&table=Table 465">DSIG/DTT_M</a> (Table 465) <li><a href="103063?version=1&table=Table 467">1/SIG*DSIG/DABS_Y_BOOST</a> (Table 467) <li><a href="103063?version=1&table=Table 469">DSIG/DABS_Y_BOOST</a> (Table 469) <li><a href="103063?version=1&table=Table 471">1/SIG*DSIG/DT1_PT</a> (Table 471) <li><a href="103063?version=1&table=Table 473">DSIG/DT1_PT</a> (Table 473) <li><a href="103063?version=1&table=Table 475">1/SIG*DSIG/DABS_TT_Y</a> (Table 475) <li><a href="103063?version=1&table=Table 477">DSIG/DABS_TT_Y</a> (Table 477) <li><a href="103063?version=1&table=Table 479">1/SIG*DSIG/DABS_T2_Y</a> (Table 479) <li><a href="103063?version=1&table=Table 481">DSIG/DABS_T2_Y</a> (Table 481) <li><a href="103063?version=1&table=Table 483">1/SIG*DSIG/DHT_TT</a> (Table 483) <li><a href="103063?version=1&table=Table 485">DSIG/DHT_TT</a> (Table 485) <li><a href="103063?version=1&table=Table 487">1/SIG*DSIG/DABS_T1_Y</a> (Table 487) <li><a href="103063?version=1&table=Table 489">DSIG/DABS_T1_Y</a> (Table 489) </ul><br/> <u>2D:</u><br/> Spectra:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 490">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 490) <li><a href="103063?version=1&table=Table 491">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 491) <li><a href="103063?version=1&table=Table 492">1/SIG*D2SIG/DABS_TT_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 492) <li><a href="103063?version=1&table=Table 499">D2SIG/DABS_TT_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 499) <li><a href="103063?version=1&table=Table 500">D2SIG/DABS_TT_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 500) <li><a href="103063?version=1&table=Table 501">D2SIG/DABS_TT_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 501) <li><a href="103063?version=1&table=Table 508">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.0 < ABS_T1_Y < 0.5 )</a> (Table 508) <li><a href="103063?version=1&table=Table 509">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.5 < ABS_T1_Y < 1.0 )</a> (Table 509) <li><a href="103063?version=1&table=Table 510">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.0 < ABS_T1_Y < 1.5 )</a> (Table 510) <li><a href="103063?version=1&table=Table 511">1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.5 < ABS_T1_Y < 2.5 )</a> (Table 511) <li><a href="103063?version=1&table=Table 522">D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.0 < ABS_T1_Y < 0.5 )</a> (Table 522) <li><a href="103063?version=1&table=Table 523">D2SIG/DABS_T2_Y/DABS_T1_Y ( 0.5 < ABS_T1_Y < 1.0 )</a> (Table 523) <li><a href="103063?version=1&table=Table 524">D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.0 < ABS_T1_Y < 1.5 )</a> (Table 524) <li><a href="103063?version=1&table=Table 525">D2SIG/DABS_T2_Y/DABS_T1_Y ( 1.5 < ABS_T1_Y < 2.5 )</a> (Table 525) <li><a href="103063?version=1&table=Table 536">1/SIG*D2SIG/DT2_PT/DM ( 0.0 GeV < M < 700.0 GeV)</a> (Table 536) <li><a href="103063?version=1&table=Table 537">1/SIG*D2SIG/DT2_PT/DM ( 700.0 GeV < M < 970.0 GeV)</a> (Table 537) <li><a href="103063?version=1&table=Table 538">1/SIG*D2SIG/DT2_PT/DM ( 970.0 GeV < M < 1315.0 GeV)</a> (Table 538) <li><a href="103063?version=1&table=Table 539">1/SIG*D2SIG/DT2_PT/DM ( 1315.0 GeV < M < 3000.0 GeV)</a> (Table 539) <li><a href="103063?version=1&table=Table 550">D2SIG/DT2_PT/DM ( 0.0 GeV < M < 700.0 GeV)</a> (Table 550) <li><a href="103063?version=1&table=Table 551">D2SIG/DT2_PT/DM ( 700.0 GeV < M < 970.0 GeV)</a> (Table 551) <li><a href="103063?version=1&table=Table 552">D2SIG/DT2_PT/DM ( 970.0 GeV < M < 1315.0 GeV)</a> (Table 552) <li><a href="103063?version=1&table=Table 553">D2SIG/DT2_PT/DM ( 1315.0 GeV < M < 3000.0 GeV)</a> (Table 553) <li><a href="103063?version=1&table=Table 564">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 564) <li><a href="103063?version=1&table=Table 565">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 565) <li><a href="103063?version=1&table=Table 566">1/SIG*D2SIG/DABS_T1_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 566) <li><a href="103063?version=1&table=Table 573">D2SIG/DABS_T1_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 573) <li><a href="103063?version=1&table=Table 574">D2SIG/DABS_T1_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 574) <li><a href="103063?version=1&table=Table 575">D2SIG/DABS_T1_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 575) <li><a href="103063?version=1&table=Table 582">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 582) <li><a href="103063?version=1&table=Table 583">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 583) <li><a href="103063?version=1&table=Table 584">1/SIG*D2SIG/DABS_T2_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 584) <li><a href="103063?version=1&table=Table 591">D2SIG/DABS_T2_Y/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 591) <li><a href="103063?version=1&table=Table 592">D2SIG/DABS_T2_Y/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 592) <li><a href="103063?version=1&table=Table 593">D2SIG/DABS_T2_Y/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 593) <li><a href="103063?version=1&table=Table 600">1/SIG*D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 600) <li><a href="103063?version=1&table=Table 601">1/SIG*D2SIG/DTT_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 601) <li><a href="103063?version=1&table=Table 602">1/SIG*D2SIG/DTT_PT/DTT_M ( 970.0 GeV < TT_M < 1315.0 GeV)</a> (Table 602) <li><a href="103063?version=1&table=Table 603">1/SIG*D2SIG/DTT_PT/DTT_M ( 1315.0 GeV < TT_M < 3000.0 GeV)</a> (Table 603) <li><a href="103063?version=1&table=Table 614">D2SIG/DTT_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 614) <li><a href="103063?version=1&table=Table 615">D2SIG/DTT_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 615) <li><a href="103063?version=1&table=Table 616">D2SIG/DTT_PT/DTT_M ( 970.0 GeV < TT_M < 1315.0 GeV)</a> (Table 616) <li><a href="103063?version=1&table=Table 617">D2SIG/DTT_PT/DTT_M ( 1315.0 GeV < TT_M < 3000.0 GeV)</a> (Table 617) <li><a href="103063?version=1&table=Table 628">1/SIG*D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 628) <li><a href="103063?version=1&table=Table 629">1/SIG*D2SIG/DT1_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 629) <li><a href="103063?version=1&table=Table 630">1/SIG*D2SIG/DT1_PT/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 630) <li><a href="103063?version=1&table=Table 637">D2SIG/DT1_PT/DTT_M ( 0.0 GeV < TT_M < 700.0 GeV)</a> (Table 637) <li><a href="103063?version=1&table=Table 638">D2SIG/DT1_PT/DTT_M ( 700.0 GeV < TT_M < 970.0 GeV)</a> (Table 638) <li><a href="103063?version=1&table=Table 639">D2SIG/DT1_PT/DTT_M ( 970.0 GeV < TT_M < 3000.0 GeV)</a> (Table 639) <li><a href="103063?version=1&table=Table 646">1/SIG*D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 170.0 GeV)</a> (Table 646) <li><a href="103063?version=1&table=Table 647">1/SIG*D2SIG/DT1_PT/DT2_PT ( 170.0 GeV < T2_PT < 290.0 GeV)</a> (Table 647) <li><a href="103063?version=1&table=Table 648">1/SIG*D2SIG/DT1_PT/DT2_PT ( 290.0 GeV < T2_PT < 450.0 GeV)</a> (Table 648) <li><a href="103063?version=1&table=Table 649">1/SIG*D2SIG/DT1_PT/DT2_PT ( 450.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 649) <li><a href="103063?version=1&table=Table 660">D2SIG/DT1_PT/DT2_PT ( 0.0 GeV < T2_PT < 170.0 GeV)</a> (Table 660) <li><a href="103063?version=1&table=Table 661">D2SIG/DT1_PT/DT2_PT ( 170.0 GeV < T2_PT < 290.0 GeV)</a> (Table 661) <li><a href="103063?version=1&table=Table 662">D2SIG/DT1_PT/DT2_PT ( 290.0 GeV < T2_PT < 450.0 GeV)</a> (Table 662) <li><a href="103063?version=1&table=Table 663">D2SIG/DT1_PT/DT2_PT ( 450.0 GeV < T2_PT < 1000.0 GeV)</a> (Table 663) </ul><br/> Covariances:<br/> <ul><br/> <li><a href="103063?version=1&table=Table 493">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 493) <li><a href="103063?version=1&table=Table 494">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 494) <li><a href="103063?version=1&table=Table 495">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 495) <li><a href="103063?version=1&table=Table 496">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 496) <li><a href="103063?version=1&table=Table 497">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 497) <li><a href="103063?version=1&table=Table 498">Matrix for 1/SIG*D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 498) <li><a href="103063?version=1&table=Table 502">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 502) <li><a href="103063?version=1&table=Table 503">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 503) <li><a href="103063?version=1&table=Table 504">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 504) <li><a href="103063?version=1&table=Table 505">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 505) <li><a href="103063?version=1&table=Table 506">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 506) <li><a href="103063?version=1&table=Table 507">Matrix for D2SIG/DABS_TT_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 507) <li><a href="103063?version=1&table=Table 512">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 1th and 1th bins of ABS_T1_Y</a> (Table 512) <li><a href="103063?version=1&table=Table 513">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 1th bins of ABS_T1_Y</a> (Table 513) <li><a href="103063?version=1&table=Table 514">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 2th bins of ABS_T1_Y</a> (Table 514) <li><a href="103063?version=1&table=Table 515">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 1th bins of ABS_T1_Y</a> (Table 515) <li><a href="103063?version=1&table=Table 516">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 2th bins of ABS_T1_Y</a> (Table 516) <li><a href="103063?version=1&table=Table 517">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 3th bins of ABS_T1_Y</a> (Table 517) <li><a href="103063?version=1&table=Table 518">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 1th bins of ABS_T1_Y</a> (Table 518) <li><a href="103063?version=1&table=Table 519">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 2th bins of ABS_T1_Y</a> (Table 519) <li><a href="103063?version=1&table=Table 520">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 3th bins of ABS_T1_Y</a> (Table 520) <li><a href="103063?version=1&table=Table 521">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 4th bins of ABS_T1_Y</a> (Table 521) <li><a href="103063?version=1&table=Table 526">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 1th and 1th bins of ABS_T1_Y</a> (Table 526) <li><a href="103063?version=1&table=Table 527">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 1th bins of ABS_T1_Y</a> (Table 527) <li><a href="103063?version=1&table=Table 528">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 2th and 2th bins of ABS_T1_Y</a> (Table 528) <li><a href="103063?version=1&table=Table 529">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 1th bins of ABS_T1_Y</a> (Table 529) <li><a href="103063?version=1&table=Table 530">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 2th bins of ABS_T1_Y</a> (Table 530) <li><a href="103063?version=1&table=Table 531">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 3th and 3th bins of ABS_T1_Y</a> (Table 531) <li><a href="103063?version=1&table=Table 532">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 1th bins of ABS_T1_Y</a> (Table 532) <li><a href="103063?version=1&table=Table 533">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 2th bins of ABS_T1_Y</a> (Table 533) <li><a href="103063?version=1&table=Table 534">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 3th bins of ABS_T1_Y</a> (Table 534) <li><a href="103063?version=1&table=Table 535">Matrix for D2SIG/DABS_T2_Y/DABS_T1_Y between the 4th and 4th bins of ABS_T1_Y</a> (Table 535) <li><a href="103063?version=1&table=Table 540">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 1th and 1th bins of M</a> (Table 540) <li><a href="103063?version=1&table=Table 541">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 2th and 1th bins of M</a> (Table 541) <li><a href="103063?version=1&table=Table 542">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 2th and 2th bins of M</a> (Table 542) <li><a href="103063?version=1&table=Table 543">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 1th bins of M</a> (Table 543) <li><a href="103063?version=1&table=Table 544">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 2th bins of M</a> (Table 544) <li><a href="103063?version=1&table=Table 545">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 3th and 3th bins of M</a> (Table 545) <li><a href="103063?version=1&table=Table 546">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 1th bins of M</a> (Table 546) <li><a href="103063?version=1&table=Table 547">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 2th bins of M</a> (Table 547) <li><a href="103063?version=1&table=Table 548">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 3th bins of M</a> (Table 548) <li><a href="103063?version=1&table=Table 549">Matrix for 1/SIG*D2SIG/DT2_PT/DM between the 4th and 4th bins of M</a> (Table 549) <li><a href="103063?version=1&table=Table 554">Matrix for D2SIG/DT2_PT/DM between the 1th and 1th bins of M</a> (Table 554) <li><a href="103063?version=1&table=Table 555">Matrix for D2SIG/DT2_PT/DM between the 2th and 1th bins of M</a> (Table 555) <li><a href="103063?version=1&table=Table 556">Matrix for D2SIG/DT2_PT/DM between the 2th and 2th bins of M</a> (Table 556) <li><a href="103063?version=1&table=Table 557">Matrix for D2SIG/DT2_PT/DM between the 3th and 1th bins of M</a> (Table 557) <li><a href="103063?version=1&table=Table 558">Matrix for D2SIG/DT2_PT/DM between the 3th and 2th bins of M</a> (Table 558) <li><a href="103063?version=1&table=Table 559">Matrix for D2SIG/DT2_PT/DM between the 3th and 3th bins of M</a> (Table 559) <li><a href="103063?version=1&table=Table 560">Matrix for D2SIG/DT2_PT/DM between the 4th and 1th bins of M</a> (Table 560) <li><a href="103063?version=1&table=Table 561">Matrix for D2SIG/DT2_PT/DM between the 4th and 2th bins of M</a> (Table 561) <li><a href="103063?version=1&table=Table 562">Matrix for D2SIG/DT2_PT/DM between the 4th and 3th bins of M</a> (Table 562) <li><a href="103063?version=1&table=Table 563">Matrix for D2SIG/DT2_PT/DM between the 4th and 4th bins of M</a> (Table 563) <li><a href="103063?version=1&table=Table 567">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 567) <li><a href="103063?version=1&table=Table 568">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 568) <li><a href="103063?version=1&table=Table 569">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 569) <li><a href="103063?version=1&table=Table 570">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 570) <li><a href="103063?version=1&table=Table 571">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 571) <li><a href="103063?version=1&table=Table 572">Matrix for 1/SIG*D2SIG/DABS_T1_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 572) <li><a href="103063?version=1&table=Table 576">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 576) <li><a href="103063?version=1&table=Table 577">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 577) <li><a href="103063?version=1&table=Table 578">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 578) <li><a href="103063?version=1&table=Table 579">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 579) <li><a href="103063?version=1&table=Table 580">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 580) <li><a href="103063?version=1&table=Table 581">Matrix for D2SIG/DABS_T1_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 581) <li><a href="103063?version=1&table=Table 585">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 585) <li><a href="103063?version=1&table=Table 586">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 586) <li><a href="103063?version=1&table=Table 587">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 587) <li><a href="103063?version=1&table=Table 588">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 588) <li><a href="103063?version=1&table=Table 589">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 589) <li><a href="103063?version=1&table=Table 590">Matrix for 1/SIG*D2SIG/DABS_T2_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 590) <li><a href="103063?version=1&table=Table 594">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 1th and 1th bins of TT_M</a> (Table 594) <li><a href="103063?version=1&table=Table 595">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 2th and 1th bins of TT_M</a> (Table 595) <li><a href="103063?version=1&table=Table 596">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 2th and 2th bins of TT_M</a> (Table 596) <li><a href="103063?version=1&table=Table 597">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 1th bins of TT_M</a> (Table 597) <li><a href="103063?version=1&table=Table 598">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 2th bins of TT_M</a> (Table 598) <li><a href="103063?version=1&table=Table 599">Matrix for D2SIG/DABS_T2_Y/DTT_M between the 3th and 3th bins of TT_M</a> (Table 599) <li><a href="103063?version=1&table=Table 604">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 604) <li><a href="103063?version=1&table=Table 605">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 605) <li><a href="103063?version=1&table=Table 606">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 606) <li><a href="103063?version=1&table=Table 607">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 607) <li><a href="103063?version=1&table=Table 608">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 608) <li><a href="103063?version=1&table=Table 609">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 609) <li><a href="103063?version=1&table=Table 610">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 610) <li><a href="103063?version=1&table=Table 611">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 611) <li><a href="103063?version=1&table=Table 612">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 612) <li><a href="103063?version=1&table=Table 613">Matrix for 1/SIG*D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 613) <li><a href="103063?version=1&table=Table 618">Matrix for D2SIG/DTT_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 618) <li><a href="103063?version=1&table=Table 619">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 619) <li><a href="103063?version=1&table=Table 620">Matrix for D2SIG/DTT_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 620) <li><a href="103063?version=1&table=Table 621">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 621) <li><a href="103063?version=1&table=Table 622">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 622) <li><a href="103063?version=1&table=Table 623">Matrix for D2SIG/DTT_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 623) <li><a href="103063?version=1&table=Table 624">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 1th bins of TT_M</a> (Table 624) <li><a href="103063?version=1&table=Table 625">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 2th bins of TT_M</a> (Table 625) <li><a href="103063?version=1&table=Table 626">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 3th bins of TT_M</a> (Table 626) <li><a href="103063?version=1&table=Table 627">Matrix for D2SIG/DTT_PT/DTT_M between the 4th and 4th bins of TT_M</a> (Table 627) <li><a href="103063?version=1&table=Table 631">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 631) <li><a href="103063?version=1&table=Table 632">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 632) <li><a href="103063?version=1&table=Table 633">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 633) <li><a href="103063?version=1&table=Table 634">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 634) <li><a href="103063?version=1&table=Table 635">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 635) <li><a href="103063?version=1&table=Table 636">Matrix for 1/SIG*D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 636) <li><a href="103063?version=1&table=Table 640">Matrix for D2SIG/DT1_PT/DTT_M between the 1th and 1th bins of TT_M</a> (Table 640) <li><a href="103063?version=1&table=Table 641">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 1th bins of TT_M</a> (Table 641) <li><a href="103063?version=1&table=Table 642">Matrix for D2SIG/DT1_PT/DTT_M between the 2th and 2th bins of TT_M</a> (Table 642) <li><a href="103063?version=1&table=Table 643">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 1th bins of TT_M</a> (Table 643) <li><a href="103063?version=1&table=Table 644">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 2th bins of TT_M</a> (Table 644) <li><a href="103063?version=1&table=Table 645">Matrix for D2SIG/DT1_PT/DTT_M between the 3th and 3th bins of TT_M</a> (Table 645) <li><a href="103063?version=1&table=Table 650">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 650) <li><a href="103063?version=1&table=Table 651">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 651) <li><a href="103063?version=1&table=Table 652">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 652) <li><a href="103063?version=1&table=Table 653">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 653) <li><a href="103063?version=1&table=Table 654">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 654) <li><a href="103063?version=1&table=Table 655">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 655) <li><a href="103063?version=1&table=Table 656">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 656) <li><a href="103063?version=1&table=Table 657">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 657) <li><a href="103063?version=1&table=Table 658">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 658) <li><a href="103063?version=1&table=Table 659">Matrix for 1/SIG*D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 659) <li><a href="103063?version=1&table=Table 664">Matrix for D2SIG/DT1_PT/DT2_PT between the 1th and 1th bins of T2_PT</a> (Table 664) <li><a href="103063?version=1&table=Table 665">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 1th bins of T2_PT</a> (Table 665) <li><a href="103063?version=1&table=Table 666">Matrix for D2SIG/DT1_PT/DT2_PT between the 2th and 2th bins of T2_PT</a> (Table 666) <li><a href="103063?version=1&table=Table 667">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 1th bins of T2_PT</a> (Table 667) <li><a href="103063?version=1&table=Table 668">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 2th bins of T2_PT</a> (Table 668) <li><a href="103063?version=1&table=Table 669">Matrix for D2SIG/DT1_PT/DT2_PT between the 3th and 3th bins of T2_PT</a> (Table 669) <li><a href="103063?version=1&table=Table 670">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 1th bins of T2_PT</a> (Table 670) <li><a href="103063?version=1&table=Table 671">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 2th bins of T2_PT</a> (Table 671) <li><a href="103063?version=1&table=Table 672">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 3th bins of T2_PT</a> (Table 672) <li><a href="103063?version=1&table=Table 673">Matrix for D2SIG/DT1_PT/DT2_PT between the 4th and 4th bins of T2_PT</a> (Table 673) </ul><br/>
Relative differential cross-section as a function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology. Note that the values shown here are obtained by propagating the individual uncertainties to the measured cross-sections, while the covariance matrices are evaluated using pseudo-experiments as described in the text. The measured differential cross-section is compared with the prediction obtained with the Powheg+Pythia8 Monte Carlo generator.
Covariance matrix of the relative differential cross-section as function of $\Delta R^{extra1}_{jet1}$ at particle level in the all hadronic resolved topology, accounting for the statistical and systematic uncertainties.
This paper describes precision measurements of the transverse momentum $p_\mathrm{T}^{\ell\ell}$ ($\ell=e,\mu$) and of the angular variable $\phi^{*}_{\eta}$ distributions of Drell-Yan lepton pairs in a mass range of 66-116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13$ TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton-proton collisions at $\sqrt{s}=$7 and 8 TeV, these new measurements probe perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. They reach a precision of 0.2% for the normalized spectra at low values of $p_\mathrm{T}^{\ell\ell}$. The data are compared with different QCD predictions, where it is found that predictions based on resummation approaches can describe the full spectrum within uncertainties.
Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.
Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.
Selected signal candidate events in data for both decay channels as well as the expected background contributions including their total uncertainties.
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