cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.85744.v1/t2
title: "Table 2" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Double-differential cross section times the dimuon branching fraction of the psi(2S) meson for different ranges of pT in bins of |y| and for the full |y| &lt; 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t3
title: "Table 3" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Double-differential cross section times the dimuon branching fraction of the Y(1S) meson for different ranges of pT in bins of |y| and for the full |y| &lt; 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t4
title: "Table 4" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Double-differential cross section times the dimuon branching fraction of the Y(2S) meson for different ranges of pT in bins of |y| and for the full |y| &lt; 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t5
title: "Table 5" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Double-differential cross section times the dimuon branching fraction of the Y(3S) meson for different ranges of pT in bins of |y| and for the full |y| &lt; 1.2 range, for the unpolarized decay hypothesis. The global uncertainty in the integrated luminosity of 2.3% is not included in the systematic uncertainties.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t6
title: "Table 6" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Multiplicative scaling factors to obtain the J/psi differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, +0.10, -1) from the unpolarized cross section measurements given in Table 1.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t7
title: "Table 7" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Multiplicative scaling factors to obtain the psi(2S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, +0.03, -1) from the unpolarized cross section measurements given in Table 2.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t8
title: "Table 8" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Multiplicative scaling factors to obtain the Y(1S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT &lt; 50 GeV. For pT &gt; 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT &lt; 50 GeV.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t9
title: "Table 9" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Multiplicative scaling factors to obtain the Y(2S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT &lt; 50 GeV. For pT &gt; 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT &lt; 50 GeV.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.25549/stayathome-c125-11
title: 5 videos on the impact of COVID-19 on Cholena Humphrey

description: How does COVID-19 impact the University of Southern California community?USC Libraries makes an effort to collect and archive materials and stories from individuals from the University of Southern California, Los Angeles, and the Southern California community as a way to create a public record of the coronavirus COVID-19 pandemic that will be used for research and other purposes.Submissions will be archived and processed by USC Libraries Special Collections and USC.Libraries Digital Library. Submissions will only be viewed by the #StayAtHome project team. If you have any questions or comments please visit our website. We have an FAQ, helpful submission guidelines, and project team information with direct contact details: https://libguides.usc.edu/stayathome.There is a companion Website (https://stayathomeusc.github.io/stayathome/) to USC's #StayAtHome archiving project. The map will provide access to a selection of contributions which you can select and read more about.
DOI: 10.17182/hepdata.85744.v1/t10
title: "Table 10" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Multiplicative scaling factors to obtain the Y(3S) differential cross sections for different polarization scenarios (Lambda_{Theta} = +1, k, -1) from the unpolarized cross section measurements given in Table 3. The parameter k corresponds to a linear interpolation of the CMS measured value as a function of pT for pT &lt; 50 GeV. For pT &gt; 50 GeV, where no measurements exist, k is taken as the average of all the measured values for pT &lt; 50 GeV.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t11
title: "Table 11" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Ratio of differential cross section times branching fractions of the prompt psi(2S) to J/psi mesons assuming unpolarized productions as a function of pT for |y| &lt; 1.2.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85744.v1/t12
title: "Table 12" of "Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV"

description: Ratios of differential cross section times branching fractions of the prompt Y(2S) to Y(1S) and Y(3S) to Y(1S) mesons assuming unpolarized productions as a function of pT for |y| &lt; 1.2.
description: CERN-LHC. Differential production cross sections of prompt J/psi and psi(2S) charmonium and Y(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at sqrt(s) = 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb^−1 for the J/psi and 2.7 fb^−1 for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity |y| &lt; 1.2. The double-differential cross sections for each state are measured as a function of y and transverse momentum, and compared to theoretical expectations. In addition, ratios are presented of cross sections for prompt psi(2S) to J/psi, Y(2S) to Y(1S), and Y(3S) to Y(1S) production.

The tables below list the results of J/psi and psi(2S) differential cross section times dimuon branching fraction B in four rapidity bins for the unpolarized scenario, the unpolarized differential cross sections times B in the integrated rapidity range |y| &lt; 1.2 with the corresponding scaling factors needed to obtain the cross sections for different polarization scenarios and the ratio of the psi(2S) to J/psi cross sections for the integrated rapidity range |y| &lt; 1.2.
DOI: 10.17182/hepdata.85745.v1/t1
title: "Table 1" of "Measurement of the total and differential inclusive B(+) hadron cross sections in pp collisions at sqrt(s) = 13 TeV"

description: B+ differential production cross sections DSIG/DPT for |yB|&lt; 1.45 or |yB|&lt; 2.1, at 13 TeV. The calculations from FONLL and PYTHIA are provided. The ratio of the data at 13 TeV to the FONLL predictions and the ratios of the PYTHIA to the FONLL calculations are also given.
description: CERN-LHC. The differential cross sections for inclusive production of B+
 hadrons are measured as a function of the B+ transverse momentum
 and rapidity in pp collisions at a centre-of-mass energy of 13 TeV, using data collected by the CMS experiment that correspond
 to an integrated luminosity of 48.1 pb^−1. The measurement uses the exclusive decay channel B+ -&gt; J/psi K+, with J/psi
 mesons that decay to a pair of muons. The results show a reasonable agreement with theoretical calculations within the uncertainties.
 See Phys. Lett. B 771 (2017) 435 for more details.
DOI: 10.17182/hepdata.85745.v1/t2
title: "Table 2" of "Measurement of the total and differential inclusive B(+) hadron cross sections in pp collisions at sqrt(s) = 13 TeV"

description: B+ differential production cross sections DSIG/DETARAP for 10 &lt; ptB &lt; 100 GeV or 17 &lt; ptB &lt; 100 GeV, at 13 TeV. The calculations from FONLL and PYTHIA are provided. The ratio of the data at 13 TeV to the FONLL predictions and the ratios of the PYTHIA to the FONLL calculations are also given.
description: CERN-LHC. The differential cross sections for inclusive production of B+
 hadrons are measured as a function of the B+ transverse momentum
 and rapidity in pp collisions at a centre-of-mass energy of 13 TeV, using data collected by the CMS experiment that correspond
 to an integrated luminosity of 48.1 pb^−1. The measurement uses the exclusive decay channel B+ -&gt; J/psi K+, with J/psi
 mesons that decay to a pair of muons. The results show a reasonable agreement with theoretical calculations within the uncertainties.
 See Phys. Lett. B 771 (2017) 435 for more details.
DOI: 10.17182/hepdata.85745.v1/t3
title: "Table 3" of "Measurement of the total and differential inclusive B(+) hadron cross sections in pp collisions at sqrt(s) = 13 TeV"

description: Ratios of B+ differential production cross sections at 13 TeV and at 7 TeV as a function of ptB for |yB|&lt; 1.45 or |yB|&lt; 2.1. The calculations from FONLL and PYTHIA are provided as well.
description: CERN-LHC. The differential cross sections for inclusive production of B+
 hadrons are measured as a function of the B+ transverse momentum
 and rapidity in pp collisions at a centre-of-mass energy of 13 TeV, using data collected by the CMS experiment that correspond
 to an integrated luminosity of 48.1 pb^−1. The measurement uses the exclusive decay channel B+ -&gt; J/psi K+, with J/psi
 mesons that decay to a pair of muons. The results show a reasonable agreement with theoretical calculations within the uncertainties.
 See Phys. Lett. B 771 (2017) 435 for more details.
DOI: 10.17182/hepdata.85745.v1/t4
title: "Table 4" of "Measurement of the total and differential inclusive B(+) hadron cross sections in pp collisions at sqrt(s) = 13 TeV"

description: Ratios of B+ differential production cross sections at 13 TeV and at 7 TeV as a function of |yB| for 10 &lt; ptB &lt; 100 GeV or 17 &lt; ptB &lt; 100 GeV. The calculations from FONLL and PYTHIA are provided as well.
description: CERN-LHC. The differential cross sections for inclusive production of B+
 hadrons are measured as a function of the B+ transverse momentum
 and rapidity in pp collisions at a centre-of-mass energy of 13 TeV, using data collected by the CMS experiment that correspond
 to an integrated luminosity of 48.1 pb^−1. The measurement uses the exclusive decay channel B+ -&gt; J/psi K+, with J/psi
 mesons that decay to a pair of muons. The results show a reasonable agreement with theoretical calculations within the uncertainties.
 See Phys. Lett. B 771 (2017) 435 for more details.