cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.99906.v1/t63
title: "Table 63" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: MC generator filter efficiencies of the DMt samples in the tW1L channel. The maps include all samples in the $m_H - tan\beta$ plane with $m_a = 250~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t64
title: "Table 64" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: MC generator filter efficiencies of the DMt samples in the tW2L channel. The maps include all samples in the $m_a - m_H$ plane with $tan\beta = 1$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t65
title: "Table 65" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: MC generator filter efficiencies of the DMt samples in the tW2L channel. The maps include all samples in the $m_H - tan\beta$ plane with $m_a = 250~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t66
title: "Table 66" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: MC generator filter efficiencies of the DMt samples in the tj1L channel. The map includes all samples in the $m_H - tan\beta$ plane with $m_a = 250~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t67
title: "Table 67" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Background-only fit results for the tW1L and tW2L signal regions. The backgrounds which contribute only a small amount (rare processes such as triboson, Higgs boson production processes, $t\bar{t}t\bar{t}$, $t\bar{t}WW$ and non-prompt or misidentified leptons background) are grouped and labelled as ``Others´´. The quoted uncertainties on the fitted SM background include both the statistical and systematic uncertainties.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t68
title: "Table 68" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Background-only fit results for the tj1L signal regions. The backgrounds which contribute only a small amount ($Z$+jets, rare processes such as $tWZ$, triboson, Higgs boson production processes, ,$t\bar{t}t\bar{t}$, $t\bar{t}WW$) are grouped and labelled as ``Others´´. The quoted uncertainties on the fitted SM background include both the statistical and systematic uncertainties.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t69
title: "Table 69" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Cutflow of the weighted events with statistical uncertainties for two DMt samples in all bins of the tW1L channel. The PreSelection includes at least 1 lepton in the event, at least 1 $b$-jet with $p_{\mathrm{T}} &gt; 50~GeV$, $m\mathrm{_{T}^{lep}} &gt; 30~GeV$, $\Delta\phi\mathrm{_{4jets, MET}^{min}} &gt; 0.5$ and $E\mathrm{_{T}^{miss}} &gt; 200~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t70
title: "Table 70" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Cutflow of the weighted events with statistical uncertainties for two DMt samples in the tW2L channel. The PreSelection includes at least 2 leptons in the event, at least 1 $b$-jet with $p_{\mathrm{T}} &gt; 40~GeV$, $m_{ll} &gt; 40~GeV$, $m\mathrm{_{T2}} &gt; 40~GeV$, $\Delta\phi\mathrm{_{4jets, MET}^{min}} &gt; 0.5$ and $E\mathrm{_{T}^{miss}} &gt; 200~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99906.v1/t71
title: "Table 71" of "Search for dark matter produced in association with a single top quark in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Cutflow of the weighted events with the statistical uncertainties (except for the first cuts) for two DMt samples in all bins off the tj1L channel. The PreSelection includes at least 1 lepton in the event, at least 1 $b$-jet with $p_{\mathrm{T}} &gt; 50~GeV$, $m\mathrm{_{T}^{lep}} &gt; 30~GeV$, $\Delta\phi\mathrm{_{4jets, MET}^{min}} &gt; 0.5$ and $E\mathrm{_{T}^{miss}} &gt; 200~GeV$.
description: CERN-LHC, ATLAS. A search for dark matter in the context of a two-Higgs-doublet model together with an additional pseudo-scalar mediator, which decays to the dark matter particles is presented. Processes where the pseudo-scalar mediator is produced in association with a single top quark are explored for the first time at the LHC. Several final states are considered, including either one or two charged leptons (electrons or muons) and a significant amount of missing transverse momentum. The analysis is based on the data collected with the ATLAS experiment at $\sqrt{s} = 13$ TeV during LHC Run 2 ($2015-2018$), corresponding to an integrated luminosity of 139 fb$^{-1}$.
DOI: 10.17182/hepdata.99928.v1/t1
title: "Table 1" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t2
title: "Table 2" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t3
title: "Table 3" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t4
title: "Table 4" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t5
title: "Table 5" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t10
title: "Table 10" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t11
title: "Table 11" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t12
title: "Table 12" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t6
title: "Table 6" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t7
title: "Table 7" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t8
title: "Table 8" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t9
title: "Table 9" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99928.v1/t13
title: "Table 13" of "$\rm{K}^{*}(\rm{892})^{0}$ and $\phi(1020)$ production at midrapidity in pp collisions at $\sqrt{s}$ = 8 TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.99929.v1/t1
title: "The dimuon mass distributions" of "Search for a narrow resonance lighter than 200 GeV decaying to a pair of muons in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: The dimuon mass distributions of events selected with the standard muon triggers (maroon, darker), and the scouting dimuon triggers (green, lighter). Events are required to pass all the selection requirements.
description: A search is presented for a narrow resonance decaying to a pair of oppositely charged muons using $\sqrt{s}=13$ TeV proton-proton collision data recorded at the LHC. In the 45--75 and 110--200 GeV resonance mass ranges, the search is based on conventional triggering and event reconstruction techniques. In the 11.5--45 GeV mass range, the search uses data collected with dimuon triggers with low transverse momentum thresholds, recorded at high rate by storing a reduced amount of trigger-level information. The data correspond to integrated luminosities of 137 $\mathrm{fb}^{-1}$ and 96.6 $\mathrm{fb}^{-1}$ for conventional and high-rate triggering, respectively. No significant resonant peaks are observed in the probed mass ranges. The search sets the most stringent constraints to date on a dark photon in the $\sim$30--75 and 110--200 GeV mass ranges.
DOI: 10.17182/hepdata.99929.v1/t2
title: "Expected and observed limits on $\sigma$ x $\mathcal{B}$ x $A$" of "Search for a narrow resonance lighter than 200 GeV decaying to a pair of muons in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed upper limits at 95% CL on the product of the signal cross section ($\sigma$) for a narrow resonance, branching fraction to a pair of muons ($\mathcal{B}$), and acceptance ($A$) as a function of the mass of a narrow resonance. Results obtained using the scouting (standard) triggers are to the left (right) of the vertical purple line.
description: A search is presented for a narrow resonance decaying to a pair of oppositely charged muons using $\sqrt{s}=13$ TeV proton-proton collision data recorded at the LHC. In the 45--75 and 110--200 GeV resonance mass ranges, the search is based on conventional triggering and event reconstruction techniques. In the 11.5--45 GeV mass range, the search uses data collected with dimuon triggers with low transverse momentum thresholds, recorded at high rate by storing a reduced amount of trigger-level information. The data correspond to integrated luminosities of 137 $\mathrm{fb}^{-1}$ and 96.6 $\mathrm{fb}^{-1}$ for conventional and high-rate triggering, respectively. No significant resonant peaks are observed in the probed mass ranges. The search sets the most stringent constraints to date on a dark photon in the $\sim$30--75 and 110--200 GeV mass ranges.
DOI: 10.17182/hepdata.99929.v1/t3
title: "Expected and observed limits on $\epsilon^{2}$" of "Search for a narrow resonance lighter than 200 GeV decaying to a pair of muons in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed upper limits at 90% CL on $\epsilon^{2}$, the square of the kinetic mixing coefficient, as a function of the dark photon mass. Results obtained using the scouting (standard) triggers are to the left (right) of the vertical purple line.
description: A search is presented for a narrow resonance decaying to a pair of oppositely charged muons using $\sqrt{s}=13$ TeV proton-proton collision data recorded at the LHC. In the 45--75 and 110--200 GeV resonance mass ranges, the search is based on conventional triggering and event reconstruction techniques. In the 11.5--45 GeV mass range, the search uses data collected with dimuon triggers with low transverse momentum thresholds, recorded at high rate by storing a reduced amount of trigger-level information. The data correspond to integrated luminosities of 137 $\mathrm{fb}^{-1}$ and 96.6 $\mathrm{fb}^{-1}$ for conventional and high-rate triggering, respectively. No significant resonant peaks are observed in the probed mass ranges. The search sets the most stringent constraints to date on a dark photon in the $\sim$30--75 and 110--200 GeV mass ranges.
DOI: 10.17182/hepdata.100086.v1/t1
title: "Table 1" of "J/psi suppression at forward rapidity in Au+Au collisions at sqrt(s_NN)=200 GeV"

description: J/psi invariant yield in Au+Au collisions as a function of $N_{part}$ at forward rapidity ($p_{T}$ integrated). The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Heavy quarkonia are observed to be suppressed in relativistic heavy ion collisions relative to their production in p$+$p collisions scaled by the number of binary collisions. In order to determine if this suppression is related to color screening of these states in the produced medium, one needs to account for other nuclear modifications including those in cold nuclear matter. In this paper, we present new measurements from the PHENIX 2007 data set of J/$\psi$ yields at forward rapidity ($1.2&lt;|y|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The data confirm the earlier finding that the suppression of J/$\psi$ at forward rapidity is stronger than at midrapidity, while also extending the measurement to finer bins in collision centrality and higher transverse momentum ($p_{T}$). We compare the experimental data to the most recent theoretical calculations that incorporate a variety of physics mechanisms including gluon saturation, gluon shadowing, initial-state parton energy loss, cold nuclear matter breakup, color screening, and charm recombination. We find J/$\psi$ suppression beyond cold-nuclear-matter effects. However, the current level of disagreement between models and d$+$Au data precludes using these models to quantify the hot-nuclear-matter suppression.
DOI: 10.17182/hepdata.100086.v1/t2
title: "Table 2" of "J/psi suppression at forward rapidity in Au+Au collisions at sqrt(s_NN)=200 GeV"

description: J/psi nuclear modification $R_{AA}$ in Au+Au collisions as a function of $N_{part}$ at forward rapidity ($p_T$ integrated). The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Heavy quarkonia are observed to be suppressed in relativistic heavy ion collisions relative to their production in p$+$p collisions scaled by the number of binary collisions. In order to determine if this suppression is related to color screening of these states in the produced medium, one needs to account for other nuclear modifications including those in cold nuclear matter. In this paper, we present new measurements from the PHENIX 2007 data set of J/$\psi$ yields at forward rapidity ($1.2&lt;|y|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The data confirm the earlier finding that the suppression of J/$\psi$ at forward rapidity is stronger than at midrapidity, while also extending the measurement to finer bins in collision centrality and higher transverse momentum ($p_{T}$). We compare the experimental data to the most recent theoretical calculations that incorporate a variety of physics mechanisms including gluon saturation, gluon shadowing, initial-state parton energy loss, cold nuclear matter breakup, color screening, and charm recombination. We find J/$\psi$ suppression beyond cold-nuclear-matter effects. However, the current level of disagreement between models and d$+$Au data precludes using these models to quantify the hot-nuclear-matter suppression.
DOI: 10.17182/hepdata.100086.v1/t3
title: "Table 3" of "J/psi suppression at forward rapidity in Au+Au collisions at sqrt(s_NN)=200 GeV"

description: J/psi invariant yield in Au+Au collisions as a function of transverse momentum for the 0-20% centrality class at forward rapidity. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.
description: BNL-RHIC. Heavy quarkonia are observed to be suppressed in relativistic heavy ion collisions relative to their production in p$+$p collisions scaled by the number of binary collisions. In order to determine if this suppression is related to color screening of these states in the produced medium, one needs to account for other nuclear modifications including those in cold nuclear matter. In this paper, we present new measurements from the PHENIX 2007 data set of J/$\psi$ yields at forward rapidity ($1.2&lt;|y|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The data confirm the earlier finding that the suppression of J/$\psi$ at forward rapidity is stronger than at midrapidity, while also extending the measurement to finer bins in collision centrality and higher transverse momentum ($p_{T}$). We compare the experimental data to the most recent theoretical calculations that incorporate a variety of physics mechanisms including gluon saturation, gluon shadowing, initial-state parton energy loss, cold nuclear matter breakup, color screening, and charm recombination. We find J/$\psi$ suppression beyond cold-nuclear-matter effects. However, the current level of disagreement between models and d$+$Au data precludes using these models to quantify the hot-nuclear-matter suppression.