cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.155514.v1/t6
title: "Table 6" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^0$ $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t8
title: "Table 8" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\mathrm{D}^+$ / non-prompt $\mathrm{D}^0$ yield ratio in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155514.v1/t9
title: "Table 9" of "Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV"

description: Non-prompt $\Lambda_{c}^{+}$ / non-prompt $\mathrm{D}^0$ yield ratio in p--Pb collisions at $\sqrt{{s_\mathrm{NN}}}=5.02~\mathrm{{TeV}}$ in the rapidity interval $-0.96 &lt; y_{\mathrm{cms}} &lt; 0.04$.
description: The production cross sections of $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ hadrons originating from beauty-hadron decays(i.e. non-prompt) were measured for the first time at midrapidity in proton--lead (p--Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{{s_\mathrm{NN}}}=5.02 \mathrm{{TeV}}$. Nuclear modification factors ($R_{\mathrm{pPb}}$) of non-prompt $\mathrm{D}^0$, $\mathrm{D}^+$, and $\Lambda_{c}^{+}$ are calculated as a function of the transverse momentum ($p_\mathrm{{T}}$)to investigate the modification of the momentum spectra measured in p--Pb collisions with respect to those measured in proton-proton (pp) collisions at the same energy. The $R_{\mathrm{pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_\mathrm{{T}}$ dependence. The $p_\mathrm{{T}}$-integrated cross sections and $p_\mathrm{{T}}$-integrated $R_{\mathrm{pPb}}$ of non-prompt $\mathrm{D}^0$ and $\mathrm{D}^+$ mesons are also computed by extrapolating the visible cross sections down to $p_\mathrm{{T}}$ = 0.The non-prompt D-meson $R_{\mathrm{pPb}}$ integrated over $p_\mathrm{{T}}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\Lambda_{c}^{+}/\mathrm{D}^0$ and $\mathrm{D}^+/\mathrm{D}^0$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_\mathrm{{T}}$ display a similar trend to that measured for charm hadrons in the same collision system.
DOI: 10.17182/hepdata.155565.v1/t1
title: "Figure 1 (a)" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-normalized $J/\psi$ yields as a function of self-normalized $N_{ch}$ for the same arm before subtraction
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155565.v1/t2
title: "Figure 1 (b)" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-normalized $J/\psi$ yields as a function of self-normalized $N_{ch}$ for the same arm after subtraction
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155565.v1/t3
title: "Figure 1 (c)" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-normalized $J/\psi$ yields as a function of self-normalized $N_{ch}$ for opposite arms
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155565.v1/t4
title: "Figure 2" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-Normalized $J/\psi$ yields in the same arms before and after dimuon subtraction and the comparison with PYTHIA 8 simulations
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155565.v1/t5
title: "Figure 3 (a)" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-normalized $\psi(2S)$ to $J/\psi$ yields ratio as a function of Self-normalized $N_{ch}$ in the same arms
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155565.v1/t6
title: "Figure 3 (b)" of "Multiplicity dependent $J/\psi$ and $\psi(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV"

description: Self-normalized $\psi(2S)$ to $J/\psi$ yields ratio as a function of Self-normalized $N_{ch}$ in opposite arms
description: BNL-RHIC. The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics (QCD) in high-energy hadronic interactions. However, a complete understanding of the charmonium production mechanism has not yet been achieved. Recent measurements of $J/\psi$ production as a function of event charged particle multiplicity at both LHC and RHIC energies show enhanced $J/\psi$ production yields with increasing multiplicity. One potential explanation for this type of dependence is Multi-Parton Interactions (MPI). We carry out the first measurements of self-normalized $J/\psi$ yields and the $\psi(2S)$ to $J/\psi$ ratio at both forward and backward rapidities as a function of self-normalized charged particle multiplicity in $pp$ collisions at $\sqrt{s}$ = 200 GeV. In addition, detailed PYTHIA studies tuned to RHIC energies have been performed to investigate the MPI impacts. We find that the PHENIX data are consistent with recent LHC measurements and can only be described by PYTHIA calculations that include MPI effects. The forward and backward $\psi(2S)$/$J/\psi$ ratio, which serves as a unique and powerful approach to study final state effects on charmonium production, is found to be less dependent on the charged particle multiplicity.
DOI: 10.17182/hepdata.155627.v1/t1
title: "Postfit_pulls_constraints_impacts_W" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (both nominal and 'global') for all nuisance parameters in the W boson mass fit, sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t2
title: "Postfit_pulls_constraints_impacts_W_massDiffCharge" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (both nominal and 'global') for all nuisance parameters in the W boson mass fit (charge difference), sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t3
title: "Postfit_pulls_constraints_impacts_Zwlike" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (both nominal and 'global') for all nuisance parameters in the W-like Z boson mass fit, sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t4
title: "Postfit_pulls_constraints_impacts_Zwlike_flipEventSplit" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (both nominal and 'global') for all nuisance parameters in the W-like Z boson mass fit (flip odd/even events to choose muon charge), sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t10
title: "diffXsec_Zwlike_pt" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: $d\sigma^{Z}/d\mathit{p}_{T}\ (pb\,/\,GeV)$: Unfolded measured $\mathit{p}_{T}^{Z}$ distribution compared with the generator-level predictions before the likelihood fit or after the W-like $\mathit{m}_{Z}$ fit or from the direct fit to the $(\mathit{p}_{T}^{μμ},\mathit{y}^{μμ})$ distribution. The measured cross section in each bin is reported after dividing the value by the corresponding bin width.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t11
title: "diffXsec_W_pt_helFit" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: $d\sigma^{W}/d\mathit{p}_{T}\ (pb\,/\,GeV)$: Generator-level $\mathit{p}_{T}^{W}$ distribution and uncertainty, before and after running the helicity fit. The measured cross section in each bin is reported after dividing the value by the corresponding bin width.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t5
title: "Postfit_pulls_constraints_impacts_Zwlike_massDiffCharge" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (both nominal and 'global') for all nuisance parameters in the W-like Z boson mass fit (charge difference), sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t6
title: "Postfit_pulls_constraints_impacts_Zdilepton" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (only nominal) for all nuisance parameters in the Z boson mass fit (using dimuon mass), sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t7
title: "Postfit_pulls_constraints_impacts_W_helFit" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Postfit pulls, constraints, and impacts (only nominal) for all nuisance parameters in the W boson mass fit (helicity cross section fit), sorted by the absolute value of the nominal impact.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t8
title: "diffXsec_W_pt" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: $d\sigma^{W}/d\mathit{p}_{T}\ (pb\,/\,GeV)$: Generator-level $\mathit{p}_{T}^{W}$ distribution and uncertainty. The last column reports the result of a simultaneous fit to the single muon $(\mathit{p}_{T}^{μ}, \mathit{\eta}^{μ}, \mathit{q}^{μ})$ distribution in $W$ boson decays and the dimuon $(\mathit{p}_{T}^{μμ},\mathit{y}^{μμ})$ distribution in $Z$ boson events. The measured cross section in each bin is reported after dividing the value by the corresponding bin width.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t9
title: "diffXsec_Zwlike_y" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: $d\sigma^{Z}/d|\mathit{y}|\ (pb)$: Unfolded measured $\mathit{y}^{Z}$ distribution compared with the generator-level predictions before the likelihood fit or after the W-like $\mathit{m}_{Z}$ fit or from the direct fit to the $(\mathit{p}_{T}^{μμ},\mathit{y}^{μμ})$ distribution. The measured cross section in each bin is reported after dividing the value by the corresponding bin width.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t12
title: "diffXsec_W_y_helFit" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: $d\sigma^{W}/d|\mathit{y}|\ (pb)$: Generator-level $\mathit{y}^{Z}$ distribution and uncertainty, before and after running the helicity fit. The measured cross section in each bin is reported after dividing the value by the corresponding bin width.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t13
title: "mass_summary_W_ptW_modeling" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Comparison of the nominal $\mathit{m}_{W}$ measurement and its uncertainty (total or only from $\mathit{p}_{T}^{W}$ modeling), with the alternative measurements using different approaches to the $\mathit{p}_{T}^{W}$ modeling and its uncertainty. The first column reports the measured mass for each configuration, while the second one shows the difference between the measurement and the main result.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t14
title: "mass_summary_W_pdfUnscaled" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Comparison of the nominal $\mathit{m}_{W}$ measurement and its uncertainty (total or only from the CT18Z PDF set), with the alternative measurements using different PDFs and their uncertainty before the scaling procedure described in the paper text. The measured mass values are those reported in Table A.7 of the paper. The first column reports the measured mass for each configuration, while the second one shows the difference between the measurement and the main result.
description: No data abstract available.
DOI: 10.17182/hepdata.155627.v1/t15
title: "mass_summary_W_pdfScaled" of "High-precision measurement of the W boson mass with the CMS experiment at the LHC"

description: Comparison of the nominal $\mathit{m}_{W}$ measurement and its uncertainty (total or only from the CT18Z PDF set), with the alternative measurements using different PDFs and their uncertainty after the scaling procedure described in the paper text. The measured mass values are those reported in Table A.7 of the paper. The scale factors for the PDF uncertainties from each set are reported in Table A.3 of the paper. The first column reports the measured mass for each configuration, while the second one shows the difference between the measurement and the main result.
description: No data abstract available.