cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.156187.v1/t37
title: "Figure A29-0" of "Observation of nuclear modification of energy-energy correlators inside jets in heavy ion collisions"

description: The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 1 GeV.
description: Energy-energy correlators have recently gained importance as experimental observables that have predicted sensitivities to a multitude of perturbative and nonperturbative quantum chromodynamics phenomena in high-energy collisions. Using data recorded with the CMS detector, energy-energy correlators are measured in lead-lead collisions for the first time. The data are obtained at a nucleon-nucleon center-of-mass energy of 5.02 TeV with an integrated luminosity of $1.70\,\mathrm{nb}^{-1}$. Energy-energy correlators are constructed by taking a weighted average of the separation of particle pairs ($\Delta r$) within a given jet cone of inclusive jets with transverse momenta between 120 and 200 GeV. A similar analysis is done for proton-proton collisions at the same center-of-mass energy to obtain a reference. The ratio of lead-lead to proton-proton energy-energy correlators reveals a $\Delta r$ dependence that can be related to properties of the medium created in heavy ion collisions.
DOI: 10.17182/hepdata.156187.v1/t40
title: "Figure A30-1" of "Observation of nuclear modification of energy-energy correlators inside jets in heavy ion collisions"

description: The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 1 GeV.
description: Energy-energy correlators have recently gained importance as experimental observables that have predicted sensitivities to a multitude of perturbative and nonperturbative quantum chromodynamics phenomena in high-energy collisions. Using data recorded with the CMS detector, energy-energy correlators are measured in lead-lead collisions for the first time. The data are obtained at a nucleon-nucleon center-of-mass energy of 5.02 TeV with an integrated luminosity of $1.70\,\mathrm{nb}^{-1}$. Energy-energy correlators are constructed by taking a weighted average of the separation of particle pairs ($\Delta r$) within a given jet cone of inclusive jets with transverse momenta between 120 and 200 GeV. A similar analysis is done for proton-proton collisions at the same center-of-mass energy to obtain a reference. The ratio of lead-lead to proton-proton energy-energy correlators reveals a $\Delta r$ dependence that can be related to properties of the medium created in heavy ion collisions.
DOI: 10.17182/hepdata.156187.v1/t38
title: "Figure A29-1" of "Observation of nuclear modification of energy-energy correlators inside jets in heavy ion collisions"

description: The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 1 GeV.
description: Energy-energy correlators have recently gained importance as experimental observables that have predicted sensitivities to a multitude of perturbative and nonperturbative quantum chromodynamics phenomena in high-energy collisions. Using data recorded with the CMS detector, energy-energy correlators are measured in lead-lead collisions for the first time. The data are obtained at a nucleon-nucleon center-of-mass energy of 5.02 TeV with an integrated luminosity of $1.70\,\mathrm{nb}^{-1}$. Energy-energy correlators are constructed by taking a weighted average of the separation of particle pairs ($\Delta r$) within a given jet cone of inclusive jets with transverse momenta between 120 and 200 GeV. A similar analysis is done for proton-proton collisions at the same center-of-mass energy to obtain a reference. The ratio of lead-lead to proton-proton energy-energy correlators reveals a $\Delta r$ dependence that can be related to properties of the medium created in heavy ion collisions.
DOI: 10.17182/hepdata.156187.v1/t39
title: "Figure A30-0" of "Observation of nuclear modification of energy-energy correlators inside jets in heavy ion collisions"

description: The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ &gt; 1 GeV.
description: Energy-energy correlators have recently gained importance as experimental observables that have predicted sensitivities to a multitude of perturbative and nonperturbative quantum chromodynamics phenomena in high-energy collisions. Using data recorded with the CMS detector, energy-energy correlators are measured in lead-lead collisions for the first time. The data are obtained at a nucleon-nucleon center-of-mass energy of 5.02 TeV with an integrated luminosity of $1.70\,\mathrm{nb}^{-1}$. Energy-energy correlators are constructed by taking a weighted average of the separation of particle pairs ($\Delta r$) within a given jet cone of inclusive jets with transverse momenta between 120 and 200 GeV. A similar analysis is done for proton-proton collisions at the same center-of-mass energy to obtain a reference. The ratio of lead-lead to proton-proton energy-energy correlators reveals a $\Delta r$ dependence that can be related to properties of the medium created in heavy ion collisions.
DOI: 10.17182/hepdata.156189.v1/t1
title: "bbll to dimuon 0b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel for different bbll signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t2
title: "bbll (destructive interference) to dimuon 0b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel for different bbll (destructive interference) signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t3
title: "bbll to dimuon 1b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel in 1b final state for different bbll signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t4
title: "bbll (destructive interference) to dimuon 1b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel in 1b final state for different bbll (destructive interference) signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t5
title: "bbll to dimuon 2b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel in 2b final state for different bbll signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t10
title: "bbll (destructive interference) to dielectron 1b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dielectron channel in 1b final state for different bbll (destructive interference) signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t11
title: "bbll to dielectron 2b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dielectron channel in 2b final state for different bbll signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t6
title: "bbll (destructive interference) to dimuon 2b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dimuon channel in 2b final state for different bbll (destructive interference) signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t7
title: "bbll to dielectron 0b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dielectron channel for different bbll signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.
DOI: 10.17182/hepdata.156189.v1/t8
title: "bbll (destructive interference) to dielectron 0b final state" of "Search for nonresonant new physics signals in high-mass dilepton events produced in association with b-tagged jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Signal efficiencies with Full Run 2 dielectron channel for different bbll (destructive interference) signal scenarios
description: A search for nonresonant new physics phenomena in high-mass dilepton events produced in association with b-tagged jets is performed using Run~2 proton-proton collisions data collected by the CMS experiment at the CERN LHC, at a center-of-mass energy of 13\TeV, corresponding to an integrated luminosity of 138\fbinv. The analysis considers two effective field theory models with dimension-six operators; involving four-fermion contact interactions between two leptons ($\Pell\Pell$, electrons or muons) and $\PQb$ or $\PQs$ quarks (\bbll and \bsll). Two lepton flavor combinations ($\Pe\Pe$ and $\PGm\PGm$) are required and events are classified as having 0, 1, and $\ge2$ b-tagged jets in the final state. No significant excess is observed over the standard model backgrounds. Upper limits are set on the product of production cross section of the new physics signals. These translate into lower limits on the energy scale $\Lambda$ of 6.9 to 9.0\TeV in the \bbll model, depending on model parameters, and on the ratio of energy scale and coupling of the underlying physics, \lamdagstar of 2.0 to 2.6\TeV in the \bsll model. The latter represent the most stringent limits on this model to date. Lepton flavor universality is also tested by comparing the dielectron and dimuon mass spectra for different $\PQb$-tagged jet multiplicities. No significant deviation from the standard model expectation of unity is observed.