cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.63983.v1/t85
title: "Table 85" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Signal efficiency, including the acceptance of the BDTG cut, for each point of the grid in the same flavour channel.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.63983.v1/t86
title: "Table 86" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Number of simulated events passing various stages of the selection in the hadronic mT2 analysis for a signal sample with m(STOP1)=300 GeV, m(CHARGINO1) = 150 GeV and m(NEUTRALINO1) = 50 GeV, and with the top squark decaying as STOP1 --&gt; CHARGINO1+ BOTTOM -&gt; W(*)+NEUTRALINO1+ BOTTOM with unit probability. Event weights are applied to correct simulated events to data. "Isolation" includes the effects of tight ID for electrons and the isolation selection for both electrons and muons. "Cleaning cuts" refer to cuts applied to remove non-collision backgrounds and detector noise.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.63983.v1/t87
title: "Table 87" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Number of simulated events passing various stages of the selection in the hadronic mT2 analysis for a signal sample with m(STOP1)=250 GeV, m(CHARGINO1) = 106 GeV and m(NEUTRALINO1) = 60 GeV, and with the top squark decaying as STOP1 --&gt; CHARGINO1+ BOTTOM -&gt; W(*)+NEUTRALINO1+ BOTTOM with unit probability. Event weights are applied to correct simulated events to data. "Isolation" includes the effects of tight ID for electrons and the isolation selection for both electrons and muons. "Cleaning cuts" refer to cuts applied to remove non-collision backgrounds and detector noise.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.63983.v1/t88
title: "Table 88" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Number of simulated events passing various stages of the selection in the leptonic mT2 analysis for two signal samples with the top squark decaying as STOP1 --&gt; CHARGINO1+ BOTTOM -&gt; W(*)+NEUTRALINO1+BOTTOM with unit probability. Event weights are applied to correct simulated events to data. "Isolation" includes the effects of tight ID for electrons and the isolation selection for both electrons and muons. "Cleaning cuts" refer to cuts applied to remove non-collision backgrounds and detector noise.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.63983.v1/t89
title: "Table 89" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Number of simulated events passing various stages of the selection in the leptonic mT2 analysis for a signal sample with m(STOP1)=180 GeV and m(NEUTRALINO1) = 60 GeV, and with the top squark decaying as STOP1 --&gt; W + BOTTOM + NEUTRALINO1 with unit probability. Event weights are applied to correct simulated events to data. "Isolation" includes the effects of tight ID for electrons and the isolation selection for both electrons and muons. "Cleaning cuts" refer to cuts applied to remove non-collision backgrounds and detector noise.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.63983.v1/t90
title: "Table 90" of "Search for direct top-squark pair production in final states with two leptons in pp collisions at sqrt(s)=8TeV with the ATLAS detector"

description: Number of simulated events passing various stages of the selection in the in the MVA analysis for all signal samples used to train the BDTG and with the top squark decaying as STOP1 --&gt; TOP + NEUTRALINO1 with unit probability. Event weights are applied to correct simulated events to data. "Isolation" includes the effects of tight ID for electrons and the isolation selection for both electrons and muons. "Cleaning cuts" refer to cuts applied to remove non-collision backgrounds and detector noise. The index i in category (Ci) is the one reported in table 3 for each signal point, SF and DF.
description: CERN-LHC. A search is presented for direct top-squark pair production in final states with two leptons (electrons or muons) of opposite charge using 20.3 fb^-1 of pp collision data at sqrt(s) = 8 TeV, collected by the ATLAS experiment at the Large Hadron Collider in 2012. No excess over the Standard Model expectation is found. The results are interpreted under the separate assumptions (i) that the top squark decays to a b-quark in addition to an on-shell chargino whose decay occurs via a real or virtual W boson, or (ii) that the top squark decays to a t-quark and the lightest neutralino. A top squark with a mass between 150 GeV and 445 GeV decaying to a b-quark and an on-shell chargino is excluded at 95% confidence level for a top squark mass equal to the chargino mass plus 10 GeV, in the case of a 1 GeV lightest neutralino. Top squarks with masses between 215 (90) GeV and 530 (170) GeV decaying to an on-shell (off-shell) t-quark and a neutralino are excluded at 95% confidence level for a 1 GeV neutralino.
DOI: 10.17182/hepdata.64030.v1/t1
title: "Table 1" of "Measurement of electrons from semileptonic heavy-flavor hadron decays in pp collisions at $\sqrt{s} = 2.76$ TeV"

description: Double-differential cross section for the production of electrons, i.e. (electron + positron)/2, from heavy-flavour hadron decays as a function of transverse momentum at mid-rapidity. The systematic uncertainties do not include an additional normalization uncertainty of 1.9%.
description: CERN-LHC. The $p_{\rm T}$-differential production cross section of electrons from semileptonic decays of heavy-flavor hadrons has been measured at mid-rapidity in proton-proton collisions at $\sqrt{s} = 2.76$ TeV in the transverse momentum range 0.5 &lt; $p_{\rm T}$ &lt; 12 GeV with the ALICE detector at the LHC. The analysis was performed using minimum bias events and events triggered by the electromagnetic calorimeter. Predictions from perturbative QCD calculations agree with the data within the theoretical and experimental uncertainties.
DOI: 10.17182/hepdata.64123.v1/t1
title: "Table 1" of "Measurement of the Forward-Backward Asymmetry in Top Quark-Antiquark Production in $p\bar{p}$ Collisions using the Lepton+Jets Channel"

description: Production-level forward-backward asymmetry as a function of the absolute difference in rapidity of the top quark and antiquark. The measured values are calibrated and listed with their total uncertainties. The theoretical predictions are based on MC@NLO simulation.
description: Fermilab-Tevatron. A measurement of the forward-backward asymmetry in top quark-antiquark production. The analysis uses the full Tevatron Run II (2001-2011) dataset collected by the D0 experiment at Fermilab corresponding to 9.7 fb^{-1} of proton-antiproton collisions at sqrt(s) = 1.96 TeV. The measurement is performed in lepton+jets final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be 10.6 +- 3.0 %. Results are consistent with the standard model predictions which range from 5.0% to 8.8%. The dependence of the asymmetry on the invariant mass of the top quark-antiquark system and the difference in rapidities of top quark and antiquark are presented.
DOI: 10.17182/hepdata.64123.v1/t2
title: "Table 2" of "Measurement of the Forward-Backward Asymmetry in Top Quark-Antiquark Production in $p\bar{p}$ Collisions using the Lepton+Jets Channel"

description: Production-level forward-backward asymmetry as a function of the invariant mass of the top quark-antiquark system. The measured values are calibrated and listed with their total uncertainties. The theoretical predictions are based on MC@NLO simulation.
description: Fermilab-Tevatron. A measurement of the forward-backward asymmetry in top quark-antiquark production. The analysis uses the full Tevatron Run II (2001-2011) dataset collected by the D0 experiment at Fermilab corresponding to 9.7 fb^{-1} of proton-antiproton collisions at sqrt(s) = 1.96 TeV. The measurement is performed in lepton+jets final states using a new kinematic fitting algorithm for events with four or more jets and a new partial reconstruction algorithm for events with only three jets. Corrected for detector acceptance and resolution effects, the asymmetry is evaluated to be 10.6 +- 3.0 %. Results are consistent with the standard model predictions which range from 5.0% to 8.8%. The dependence of the asymmetry on the invariant mass of the top quark-antiquark system and the difference in rapidities of top quark and antiquark are presented.
DOI: 10.17182/hepdata.64126.v1/t1
title: "Table 1" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; BOTTOM BOTTOMBAR. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64126.v1/t2
title: "Table 2" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; TAU+ TAU-. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64126.v1/t3
title: "Table 3" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; W+ W-. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64126.v1/t4
title: "Table 4" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; NUE NUEBAR. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64126.v1/t5
title: "Table 5" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; NUMU NUMUBAR. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64126.v1/t6
title: "Table 6" of "Search for neutrino emission from relic dark matter in the Sun with the Baikal NT200 detector"

description: Process: DM DM --&gt; NUTAU NUTAUBAR. Half-cone angle GAMMA, 90% upper limit N(SIGNAL) on the number of signal events, the muon flux PHI(MU), the dark matter annihilation rate in the Sun GAMMA(ANN), the dark matter-proton spin-dependent SIG(SD) and spin-independent SIG(SI) scattering cross sections and neutrino flux PHI(NU).
description: BAIKAL. We have analyzed a data set taken over 2.76 years live time with the Baikal neutrino telescope NT200. The goal of the analysis is to search for neutrinos from dark matter annihilation in the center of the Sun. Apart from the conventional annihilation channels BOTTOM BOTTOMBAR, W+ W- and TAU+ TAU- we consider also the annihilation of dark matter particles into monochromatic neutrinos. From the absence of any excess of events from the direction of the Sun over the expected background, we derive 90% upper limits on the fluxes of muons and muon neutrinos from the Sun, as well as on the elastic cross sections of dark matter scattering on protons.
DOI: 10.17182/hepdata.64151.v1/t1
title: "Table 1" of "Measurement of the differential $\gamma+2~b$-jet cross section and the ratio $\sigma$($\gamma+2~b$-jets)/$\sigma$($\gamma+b$-jet) in $p\bar{p}$ collisions at $\sqrt{s}$=1.96 TeV"

description: The differential GAMMA+2BJET production cross section, DSIG/DPT(GAMMA), in bins of PT(GAMMA).
description: Fermilab-Tevatron. We present the first measurements of the differential cross section, DSIG/DPT(GAMMA), for the production of an isolated photon in association with at least two b-quark jets. The measurements consider photons with rapidities ABS(YRAP(GAMMA)) &lt; 1.0 and transverse momenta 30 &lt; PT(GAMMA) &lt; 200 GeV. The b-quark jets are required to have PT(JET) &gt; 15 GeV and ABS(YRAP(JET)) &lt; 1.5. The ratio of differential production cross sections for GAMMA + 2 BJETs to GAMMA + BJET as a function of PT(GAMMA) is also presented. The results are based on data corresponding to 8.7 +- 0.5 fb^{-1} of proton-antiproton collisions at sqrt(s) = 1.96 TeV collected with the D0 detector from June 2006 to September 2011 at the Fermilab Tevatron Collider.
DOI: 10.17182/hepdata.64151.v1/t2
title: "Table 2" of "Measurement of the differential $\gamma+2~b$-jet cross section and the ratio $\sigma$($\gamma+2~b$-jets)/$\sigma$($\gamma+b$-jet) in $p\bar{p}$ collisions at $\sqrt{s}$=1.96 TeV"

description: The differential GAMMA+BJET production cross section, DSIG/DPT(GAMMA), in bins of PT(GAMMA).
description: Fermilab-Tevatron. We present the first measurements of the differential cross section, DSIG/DPT(GAMMA), for the production of an isolated photon in association with at least two b-quark jets. The measurements consider photons with rapidities ABS(YRAP(GAMMA)) &lt; 1.0 and transverse momenta 30 &lt; PT(GAMMA) &lt; 200 GeV. The b-quark jets are required to have PT(JET) &gt; 15 GeV and ABS(YRAP(JET)) &lt; 1.5. The ratio of differential production cross sections for GAMMA + 2 BJETs to GAMMA + BJET as a function of PT(GAMMA) is also presented. The results are based on data corresponding to 8.7 +- 0.5 fb^{-1} of proton-antiproton collisions at sqrt(s) = 1.96 TeV collected with the D0 detector from June 2006 to September 2011 at the Fermilab Tevatron Collider.
DOI: 10.17182/hepdata.64151.v1/t3
title: "Table 3" of "Measurement of the differential $\gamma+2~b$-jet cross section and the ratio $\sigma$($\gamma+2~b$-jets)/$\sigma$($\gamma+b$-jet) in $p\bar{p}$ collisions at $\sqrt{s}$=1.96 TeV"

description: The SIG(GAMMA 2BJET)/SIG(GAMMA BJET) cross section ratio in bins of PT(GAMMA).
description: Fermilab-Tevatron. We present the first measurements of the differential cross section, DSIG/DPT(GAMMA), for the production of an isolated photon in association with at least two b-quark jets. The measurements consider photons with rapidities ABS(YRAP(GAMMA)) &lt; 1.0 and transverse momenta 30 &lt; PT(GAMMA) &lt; 200 GeV. The b-quark jets are required to have PT(JET) &gt; 15 GeV and ABS(YRAP(JET)) &lt; 1.5. The ratio of differential production cross sections for GAMMA + 2 BJETs to GAMMA + BJET as a function of PT(GAMMA) is also presented. The results are based on data corresponding to 8.7 +- 0.5 fb^{-1} of proton-antiproton collisions at sqrt(s) = 1.96 TeV collected with the D0 detector from June 2006 to September 2011 at the Fermilab Tevatron Collider.