cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89881.v1/t13
title: "Table 3, au" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations, Away-side, AuAu
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t14
title: "Table 3, pp" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations, Away-side, pp
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t15
title: "Table 4" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Pi0-hadron correlations, Away-side, pp
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t16
title: "Table 5, photon" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations, Away-side, I_AA
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t17
title: "Table 5, pi0" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Pi0-hadron correlations, Away-side, I_AA
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t18
title: "Table 6, photon" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t19
title: "Table 6, pi0" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Pi0-hadron correlations
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t20
title: "Table 7, trig" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations, Away-side, I_AA (pT^trig)
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89881.v1/t21
title: "Table 7, assoc" of "Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV"

description: Direct Photon-hadron correlations, Away-side, I_AA (pT^assoc)
description: BNL-RHIC. Azimuthal correlations of charged hadrons with direct-photon ( gammadir ) and neutral-pion ( pi0 ) trigger particles are analyzed in central Au+Au and minimum-bias p+p collisions at sNN=200 GeV in the STAR experiment. The charged-hadron per-trigger yields at mid-rapidity from central Au+Au collisions are compared with p+p collisions to quantify the suppression in Au+Au collisions. The suppression of the away-side associated-particle yields per gammadir trigger is independent of the transverse momentum of the trigger particle ( pTtrig ), whereas the suppression is smaller at low transverse momentum of the associated charged hadrons ( pTassoc ). Within uncertainty, similar levels of suppression are observed for gammadir and pi0 triggers as a function of zT ( pTassoc/pTtrig ). The results are compared with energy-loss-inspired theoretical model predictions. Our studies support previous conclusions that the lost energy reappears predominantly at low transverse momentum, regardless of the trigger energy.
DOI: 10.17182/hepdata.89935.v1/t1
title: "Figure 6" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production signal strength for the different channels and their combination.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t2
title: "Figure 2" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section as a function of the k_lambda parameter.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t3
title: "Figure 3" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the production of a narrow, spin zero resonance (X) decaying into a pair of Higgs bosons.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t4
title: "Figure 4 all channels" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the different channels and their combination for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t5
title: "Figure 4 bbVV channel" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbVV channel and for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t10
title: "Figure 7" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the production of a narrow, spin two resonance (X) decaying into a pair of Higgs bosons.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t6
title: "Figure 4 bbbb channel" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbbb channel and for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t7
title: "Figure 4 bbtt channel" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbtt channel and for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t8
title: "Figure 4 bbgg channel" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbgg channel and for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89935.v1/t9
title: "Figure 5" of "Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Expected and observed 95\% \CL exclusion limits on the HH production cross section for the combination of all channels and for each benchmark model.
description: This Letter describes a search for Higgs boson pair production using the combined results from four final states: \bbgg, \bbtt, \bbbb, and \bbvv, where V represents a $\PW$ or \PZ boson. The search is performed using data collected in 2016 by the CMS experiment from LHC proton-proton collisions at $\sqrt{s} = 13\TeV$, corresponding to an integrated luminosity of 35.9\fbinv.Limits are set on the Higgs boson pair production cross section. A 95\% confidence level observed (expected) upper limit on the nonresonant production cross section is set at 22.2\,(12.8) times the standard model value.A search for narrow resonances decaying to Higgs boson pairs is also performed in the mass range 250--3000\GeV. No evidence for a signal is observed, and upper limits are set on the resonance production cross section.
DOI: 10.17182/hepdata.89936.v1/t1
title: "Figure 2a (Combination)" of "Measurement and interpretation of differential cross sections for Higgs boson production at $\sqrt{s}=$ 13 TeV"

description: Combined Higgs boson transverse momentum spectrum
description: Differential Higgs boson ($H$) production cross sections are sensitive probes for physics beyond the standard model. New physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself through deviations from the distributions predicted by the standard model. Combined spectra for the $H\to\gamma\gamma$, $H\to ZZ$, and $H\to b \overline{b}$ decay channels and the inclusive Higgs boson production cross section are presented, based on proton-proton collision data recorded with the CMS detector at $\sqrt{s}=13$\TeV corresponding to an integrated luminosity of 35.9 fb${}^{-1}$. The transverse momentum spectrum is used to place limits on the Higgs boson couplings to the top, bottom, and charm quarks, as well as its direct coupling to the gluon field. No significant deviations from the standard model are observed in any differential distribution. The measured total cross section is $61.1\pm 6.0 \text{(stat)} \pm 3.7 \text{(syst)}$ pb, and the precision of the measurement of the differential cross section of the Higgs boson transverse momentum is improved by about 15% with respect to the $H\to\gamma\gamma$ channel alone.