cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.159918.v1/t46
title: "Observed limits vs. width for $\alpha_{\mathrm{true}}$ = 0.42" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The observed 95% CL upper limits on the product of the cross section, branching fraction, and acceptance for resonant production of paired dijet resonances, X, with $\alpha_{\mathrm{true}} = M_{\mathrm{X}} / M_{\mathrm{Y}} = 0.42$ and widths of the initial resonance Y equal to 1.5, 5, and 10%. Limits are compared to predictions for scalar $\mathrm{S}_{\mathrm{uu}}$ and $\mathrm{S}_{\mathrm{dd}}$ diquarks with couplings to pairs of up and down quarks, $y_{\mathrm{uu}}$ and $y_{\mathrm{dd}}$, and to pairs of vector-like quarks, $y_{\chi}$ and $y_{\omega}$, set appropriately in order to generate the corresponding widths.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t47
title: "Local $p$-value vs. width for $\alpha_{\mathrm{true}}$ = 0.25" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed local $p$-value for a four-jet resonance, Y, decaying to a pair of dijet resonances, X, with $\alpha_{\mathrm{true}} = M_{\mathrm{X}}/M_{\mathrm{Y}}$ = 0.25, and various widths of Y superimposed.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t48
title: "Local $p$-value vs. width for $\alpha_{\mathrm{true}}$ = 0.29" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed local $p$-value for a four-jet resonance, Y, decaying to a pair of dijet resonances, X, with $\alpha_{\mathrm{true}} = M_{\mathrm{X}}/M_{\mathrm{Y}}$ = 0.29, and various widths of Y superimposed.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t49
title: "Cutflow efficiencies for $M_{\text{S}} = 2.0$ TeV" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The table presents the cumulative cutflow for a signal with $M_{\mathrm{S}} = 2.0$ TeV, $M_{\chi} = 0.5$ TeV and different width hypotheses ($\Gamma/M_{\mathrm{S}} =$ 1.5, 5, and 10%). Each row corresponds to the number of signal events that survive all cuts up to and including the one listed. The percentage in parentheses shows the efficiency of the current cut alone, defined as the ratio of the number of events that survive all cuts up to and including this one to the number of events that survived all previous cuts.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t50
title: "Cutflow efficiencies for $M_{\text{S}} = 5.0$ TeV" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The table presents the cumulative cutflow for a signal with $M_{\mathrm{S}} = 5.0$ TeV, $M_{\chi} = 1.25$ TeV and different width hypotheses ($\Gamma/M_{\mathrm{S}} =$ 1.5, 5, and 10%). Each row corresponds to the number of signal events that survive all cuts up to and including the one listed. The percentage in parentheses shows the efficiency of the current cut alone, defined as the ratio of the number of events that survive all cuts up to and including this one to the number of events that survived all previous cuts.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159918.v1/t51
title: "Cutflow efficiencies for $M_{\text{S}} = 8.6$ TeV" of "Search for resonant production of pairs of dijet resonances through broad mediators in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The table presents the cumulative cutflow for a signal with $M_{\mathrm{S}} = 8.6$ TeV, $M_{\chi} = 2.15$ TeV and different width hypotheses ($\Gamma/M_{\mathrm{S}} =$ 1.5, 5, and 10%). Each row corresponds to the number of signal events that survive all cuts up to and including the one listed. The percentage in parentheses shows the efficiency of the current cut alone, defined as the ratio of the number of events that survive all cuts up to and including this one to the number of events that survived all previous cuts.
description: A reinterpretation of a prior narrow-resonance search is performed to investigate the resonant production of pairs of dijet resonances via broad mediators. This analysis targets events with four resolved jets, requiring dijet invariant masses greater than $0.2~\mathrm{TeV}$ and four-jet invariant masses greater than $1.6~\mathrm{TeV}$. The search uses a data sample corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$ collected by the CMS experiment in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$. The reinterpretation considers the production of new heavy four-jet resonances, with widths ranging from 1.5 to 10% of their mass, which decay to a pair of dijet resonances. This analysis probes resonant production in the four-jet and dijet mass distributions. Upper limits at 95% confidence level and significances are reported on the production cross section of new resonances as functions of their widths and masses, between 2 and $10~\mathrm{TeV}$. In particular, at a four-jet resonance mass of $8.6~\mathrm{TeV}$, the local (global) significance ranges from 3.9 (1.6) to 3.6 (1.4) standard deviations (s.d.) as the resonance width is increased from 1.5 to 10%. This relative insensitivity to the choice of width indicates that a broad resonance is an equally valid interpretation of this excess. The broad resonance hypothesis at a resonance mass of $8.6~\mathrm{TeV}$ is supported by the presence of an event with a four-jet mass of $5.8~\mathrm{TeV}$ and an average dijet mass of $2.0~\mathrm{TeV}$. Also, we report the reinterpretation of a second effect, at a four-jet resonance mass of $3.6~\mathrm{TeV}$, which has a local (global) significance of up to 3.9 (2.2) s.d.
DOI: 10.17182/hepdata.159999.v1/t1
title: "Table" of "Centrality dependence of charged particle multiplicity at mid-rapidity in Au + Au collisions at s(NN)**(1/2) = 130-GeV"

description: For each measured centrality bin, based on percentile of the total cross-section, we show $dNch/d\eta|_{|\eta|&lt;1}$, the midrapidity charged particle density per unit of pseudorapidity, $\langle N_{part}\rangle$ , the average number of nucleons participating in the collision in the given centrality range, and the final result for $dNch/d\eta|_{|\eta|&lt;1}/( \frac{1}{2}\langle N_{part}\rangle )$, including the full error estimation.
description: BNL-RHIC. We present a measurement of the pseudorapidity density of primary charged particles near mid-rapidity in Au+Au collisions at $\sqrt{s_{NN}} =$ 130 GeV as a function of the number of participating nucleons. These results are compared to models in an attempt to discriminate between competing scenarios of particle production in heavy ion collisions.
DOI: 10.17182/hepdata.160247.v1/t1
title: "Table III part 1" of "Observation of a Three-Resonance Structure in the Cross Section of $e^+e^-\to\pi^+\pi^- h_c$"

description: Dressed cross section at the 19 XYZ-I energy points with large statistics. The table also lists the integral luminosity, the number of signal events, the weighted efficiency, the radiative correction factor, and the dressed cross section. For the dressed cross section, the first error is statistical, the second error is the systematic, and the third error comes from the input branching ratios which is the dominant one in the multiplicative systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.160247.v1/t2
title: "Table III part 2" of "Observation of a Three-Resonance Structure in the Cross Section of $e^+e^-\to\pi^+\pi^- h_c$"

description: Dressed cross section at the 25 XYZ-II energy points with lower statistics. The table also lists the integral luminosity, the number of signal events, the weighted efficiency, the radiative correction factor, and the dressed cross section. For the dressed cross section, the first error is statistical, the second error is the systematic, and the third error comes from the input branching ratios which is the dominant one in the multiplicative systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.160247.v1/t3
title: "Table IV" of "Observation of a Three-Resonance Structure in the Cross Section of $e^+e^-\to\pi^+\pi^- h_c$"

description: Dressed cross section and its upper limit at the 15 R-scan energy points with small statistics. The table also lists the integral luminosity, the number of signal events, the weighted efficiency, the radiative correction factor, and the dressed cross section. For the dressed cross section, the first error is statistical, the second error is the systematic, and the third error comes from the input branching ratios which is the dominant one in the multiplicative systematic uncertainties.
description: No data abstract available.
DOI: 10.17182/hepdata.160596.v1/t1
title: "Additional Figure 5 and Table 6" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured fiducial cross section summing VBF and ggF production modes.
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.
DOI: 10.17182/hepdata.160596.v1/t2
title: "Additional Figure 5 and Table 7 for VBF production" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured fiducial cross section of VBF and ggF production modes.
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.
DOI: 10.17182/hepdata.160596.v1/t3
title: "Additional Figure 5 and Table 7 for GGH production" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured fiducial cross section of VBF and ggF production modes.
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.
DOI: 10.17182/hepdata.160596.v1/t4
title: "Additional Figure A1 and Table 8" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured fiducial cross section of the VBF production mode.
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.
DOI: 10.17182/hepdata.160596.v1/t5
title: "Additional Figure A2" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix for fit configuration 1
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.
DOI: 10.17182/hepdata.160596.v1/t6
title: "Additional Figure A3" of "Model-independent measurement of the Higgs boson associated production with two jets and decaying to a pair of W bosons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix for fit configuration 2
description: A model-independent measurement is presented of the differential production cross section of the Higgs boson decaying into a pair of W bosons, with a final state including two jets produced in association. In the analysis, events are selected in which the decay products of the two W bosons consist of an electron, a muon, and two neutrinos. The study is based on proton-proton collision data collected with the CMS detector from 2016 to 2018, corresponding to an integrated luminosity of $138~\mathrm{fb}^{-1}$. The production cross section is measured as a function of the difference in azimuthal angle between the two jets. The differential cross section measurements are used to constrain Higgs boson couplings within the standard model effective field theory framework.