cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.85738.v1/t17
title: "Table 17" of "Medium modification of the shape of small-radius jets in central Pb-Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76\,\rm{TeV}$"

description: Ratio of fully corrected $LeSub$ distributions in $0$--$10\%$ central Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$\,TeV for $R = 0.2$ in the range of jet $p_{\mathrm{T,jet}}^{\rm ch}$ of $40$--$60$\,GeV$/c$ and PYTHIA 8 simulations. The systematic uncertainty of $LeSub$ is propagated to the ratio.
description: CERN-LHC.
A set of jet shapes for a small resolution parameter $R = 0.2$ was
measured at mid-rapidity for $0$-$10\%$ central Pb-Pb collisions at a centre-of-mass energy $\sqrt{\rm{s_{NN}}}$=2.76 TeV with the ALICE detector at the Large Hadron Collider (LHC).
This set of jet shapes includes the first radial moment or angularity, $g$; the momentum dispersion,
 $p_{\rm T}D$; and the difference between the leading and sub-leading
 constituent track transverse momentum, $LeSub$. These observables provide complementary information on the
 jet fragmentation and can constrain different aspects of the theoretical description of jet-medium interactions.
 The measured jet shapes are compared with PYTHIA calculations.
DOI: 10.17182/hepdata.85738.v1/t18
title: "Table 18" of "Medium modification of the shape of small-radius jets in central Pb-Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76\,\rm{TeV}$"

description: Ratio of fully corrected $LeSub$ distributions in
$0$--$10\%$ central Pb--Pb collisions at $\sqrt{s_{\rm NN}} =
2.76$\,TeV for $R = 0.2$ in the range of jet $p_{\mathrm{T,jet}}^{\rm
ch}$ of $40$--$60$\,GeV$/c$ and PYTHIA Perugia 11 simulations. The
systematic uncertainty of $LeSub$ is propagated to the ratio.
description: CERN-LHC.
A set of jet shapes for a small resolution parameter $R = 0.2$ was
measured at mid-rapidity for $0$-$10\%$ central Pb-Pb collisions at a centre-of-mass energy $\sqrt{\rm{s_{NN}}}$=2.76 TeV with the ALICE detector at the Large Hadron Collider (LHC).
This set of jet shapes includes the first radial moment or angularity, $g$; the momentum dispersion,
 $p_{\rm T}D$; and the difference between the leading and sub-leading
 constituent track transverse momentum, $LeSub$. These observables provide complementary information on the
 jet fragmentation and can constrain different aspects of the theoretical description of jet-medium interactions.
 The measured jet shapes are compared with PYTHIA calculations.
DOI: 10.25549/stayathome-c125-42
title: #StayAtHome 2020

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.85739.v1/t1
title: "Figure 6a" of "Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at $\sqrt{s} =$ 13 TeV"

description: Exclusion limits on the product of the production cross section and the branching fraction for a new spin-2 resonance decaying to WW, as a function of the resonance mass hypothesis.
description: A search for a new heavy particle decaying to a pair of vector bosons (WW or WZ) is presented using data from the CMS detector corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$ collected in proton-proton collisions at a centre-of-mass energy of 13 TeV in 2016. One of the bosons is required to be a W boson decaying to $e\nu$ or $\mu\nu$, while the other boson is required to be reconstructed as a single massive jet with substructure compatible with that of a highly-energetic quark pair from a W or Z boson decay. The search is performed in the resonance mass range between 1.0 and 4.5 TeV. The largest deviation from the background-only hypothesis is observed for a mass near 1.4 TeV and corresponds to a local significance of 2.5 standard deviations. The result is interpreted as an upper bound on the resonance production cross section. Comparing the excluded cross section values and the expectations from theoretical calculations in the bulk graviton and heavy vector triplet models, spin-2 WW resonances with mass smaller than 1.07 TeV and spin-1 WZ resonances lighter than 3.05 TeV, respectively, are excluded at 95% confidence level.
DOI: 10.17182/hepdata.85739.v1/t2
title: "Figure 6b" of "Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at $\sqrt{s} =$ 13 TeV"

description: Exclusion limits on the product of the production cross section and the branching fraction for a new spin-1 resonance decaying to WZ, as a function of the resonance mass hypothesis.
description: A search for a new heavy particle decaying to a pair of vector bosons (WW or WZ) is presented using data from the CMS detector corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$ collected in proton-proton collisions at a centre-of-mass energy of 13 TeV in 2016. One of the bosons is required to be a W boson decaying to $e\nu$ or $\mu\nu$, while the other boson is required to be reconstructed as a single massive jet with substructure compatible with that of a highly-energetic quark pair from a W or Z boson decay. The search is performed in the resonance mass range between 1.0 and 4.5 TeV. The largest deviation from the background-only hypothesis is observed for a mass near 1.4 TeV and corresponds to a local significance of 2.5 standard deviations. The result is interpreted as an upper bound on the resonance production cross section. Comparing the excluded cross section values and the expectations from theoretical calculations in the bulk graviton and heavy vector triplet models, spin-2 WW resonances with mass smaller than 1.07 TeV and spin-1 WZ resonances lighter than 3.05 TeV, respectively, are excluded at 95% confidence level.
DOI: 10.17182/hepdata.85739.v1/t3
title: "Additional Figure 1" of "Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at $\sqrt{s} =$ 13 TeV"

description: Signal selection efficiency times acceptance as a function of resonance mass for a spin-2 bulk graviton decaying to WW and a spin-1 W' decaying to WZ.
description: A search for a new heavy particle decaying to a pair of vector bosons (WW or WZ) is presented using data from the CMS detector corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$ collected in proton-proton collisions at a centre-of-mass energy of 13 TeV in 2016. One of the bosons is required to be a W boson decaying to $e\nu$ or $\mu\nu$, while the other boson is required to be reconstructed as a single massive jet with substructure compatible with that of a highly-energetic quark pair from a W or Z boson decay. The search is performed in the resonance mass range between 1.0 and 4.5 TeV. The largest deviation from the background-only hypothesis is observed for a mass near 1.4 TeV and corresponds to a local significance of 2.5 standard deviations. The result is interpreted as an upper bound on the resonance production cross section. Comparing the excluded cross section values and the expectations from theoretical calculations in the bulk graviton and heavy vector triplet models, spin-2 WW resonances with mass smaller than 1.07 TeV and spin-1 WZ resonances lighter than 3.05 TeV, respectively, are excluded at 95% confidence level.
DOI: 10.17182/hepdata.85740.v1/t1
title: "Table 1: Data from Figure 1 (a)" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The $\mathrm{J}/\psi\mathrm{K}^+$ invariant mass distribution in data
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t10
title: "Table 10: Results for the masses of P-wave B0s mesons" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured masses of $\mathrm{B}^{*}_{\mathrm{s2}}(5840)^0$ and $\mathrm{B}_{\mathrm{s1}}(5830)^0$ mesons
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t2
title: "Table 2: Data from Figure 1 (b)" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The $\mathrm{J}/\psi\mathrm{K}^{*0}$ invariant mass distribution in data
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t3
title: "Table 3: Data from Figure 2 (b)" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The $\mathrm{B}^+\pi^-$ invariant mass distribution of the selected candidates in data
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t4
title: "Table 4: Data from Figure 3 (a)" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: Invariant mass distribution of the selected $\mathrm{B}^+\mathrm{K}^-$ candidates in data
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t5
title: "Table 5: Data from Figure 3 (b)" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: Invariant mass distribution of the selected $\mathrm{B}^0 \mathrm{K}^{0}_{\mathrm{S}}$ candidates in data
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t6
title: "Table 6: Data from Table 2 of the publication" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The observed signal yields ($N$), natural widths ($\Gamma$), and mass differences from the fits to the $m_{\mathrm{BK}}$ distributions in data, for the two channels: $\mathrm{B}^+\mathrm{K}^-$ and $\mathrm{B}^0 \mathrm{K}^{0}_{\mathrm{S}}$. The uncertainties are statistical only.
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t7
title: "Table 7: Results for the braching fraction ratios" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured ratios of branching fractions
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t8
title: "Table 8: Mesured cross sections times braching fraction ratios" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured ratios of cross sections times branching fractions
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t9
title: "Table 9: Results for the mass differences" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured mass differences $M(\mathrm{B}^{(*)0}_{\mathrm{s1,2}})-M^{\mathrm{PDG}}_{\mathrm{B}}-M^{\mathrm{PDG}}_{\mathrm{K}}$
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t11
title: "Table 11: Results for the mass differences" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured mass differences between neutral and charged B mesons
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85740.v1/t12
title: "Table 12: Result for the Bs*2(5840)0 natural width" of "Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV"

description: The measured $\mathrm{B}^{*}_{\mathrm{s2}}(5840)^0$ natural width
description: CERN-LHC-CMS. Studies of Bs*2(5840)0 and Bs1(5830)0 mesons in their decays into B(*)+K- and, for the first time, B(*)0 K0s.
DOI: 10.17182/hepdata.85741.v1/t1
title: "Figure 5a" of "Angular analysis of the decay B$^+$$\to$ K$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV"

description: Figure 5a. Results of the $A_{FB}$ measurements in ranges of q2. 0 ≤ $F_{H}$ ≤ 3 and |$A_{FB}$| ≤ min(1, $F_{H}$/2).
description: CERN-LHC. CMS. The angular distribution of the flavor-changing neutral current decay B+ to K+ μ+ μ- is studied in proton-proton collisions at a center-of-mass energy of 8 TeV. The analysis is based on data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 20.5$fb^{-1}$. The forward-backward asymmetry $A_{FB}$ of the dimuon system and the contribution $F_{H}$ from the pseudoscalar, scalar, and tensor amplitudes to the decay width are measured as a function of the dimuon mass squared. The measurements are consistent with the standard model expectations.
DOI: 10.17182/hepdata.85741.v1/t2
title: "Figure 5b" of "Angular analysis of the decay B$^+$$\to$ K$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV"

description: Figure 5b. Results of the $F_{H}$ measurements in ranges of q2. 0 ≤ $F_{H}$ ≤ 3 and |$A_{FB}$| ≤ min(1, $F_{H}$/2).
description: CERN-LHC. CMS. The angular distribution of the flavor-changing neutral current decay B+ to K+ μ+ μ- is studied in proton-proton collisions at a center-of-mass energy of 8 TeV. The analysis is based on data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 20.5$fb^{-1}$. The forward-backward asymmetry $A_{FB}$ of the dimuon system and the contribution $F_{H}$ from the pseudoscalar, scalar, and tensor amplitudes to the decay width are measured as a function of the dimuon mass squared. The measurements are consistent with the standard model expectations.
DOI: 10.17182/hepdata.85741.v1/t3
title: "Table 2" of "Angular analysis of the decay B$^+$$\to$ K$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV"

description: Table 2. Results of the fit for each q2 range, together with several SM predictions. The inclusive $q^{2}$ = 1.00–22.00 $GeV^{2}$ range in the bottom line does not include events from the J/ψ and ψ(2S) resonance regions.
description: CERN-LHC. CMS. The angular distribution of the flavor-changing neutral current decay B+ to K+ μ+ μ- is studied in proton-proton collisions at a center-of-mass energy of 8 TeV. The analysis is based on data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 20.5$fb^{-1}$. The forward-backward asymmetry $A_{FB}$ of the dimuon system and the contribution $F_{H}$ from the pseudoscalar, scalar, and tensor amplitudes to the decay width are measured as a function of the dimuon mass squared. The measurements are consistent with the standard model expectations.
DOI: 10.17182/hepdata.85742.v1/t2
title: "Table 2" of "Observation of the $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) and measurement of their masses"

description: Observation of the $\chi_{b1}(3P)$ and $\chi_{b2}(3P)$ and mass splitting measurement.
description: CERN-LHC. The $\chi_{b1}(3P)$ and $\chi_{b2}(3P)$ states are observed through their $\Upsilon(3S)$ $\gamma$ decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0 fb$^{-1}$. The $\Upsilon(3S)$ mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e+e- pairs in the silicon tracker, leading to a $\chi_{b}(3P)$ mass resolution of 2.2 MeV. This is the first time that the J=1 and 2 states are well resolved and their masses individually measured: 10513.42$\pm$0.41(stat)$\pm$0.18(syst) MeV and 10524.02$\pm$0.57(stat)$\pm$0.18(syst) MeV; they are determined with respect to the world-average value of the $\Upsilon(3S)$ mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60$\pm$0.64(stat)$\pm$0.17(syst) MeV.
DOI: 10.25549/stayathome-c125-8
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.85742.v1/t1
title: "Table 1" of "Observation of the $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) and measurement of their masses"

description: Observation of the $\chi_{b1}(3P)$ and $\chi_{b2}(3P)$ and measurement of their masses.
description: CERN-LHC. The $\chi_{b1}(3P)$ and $\chi_{b2}(3P)$ states are observed through their $\Upsilon(3S)$ $\gamma$ decays, using an event sample of proton-proton collisions collected by the CMS experiment at the CERN LHC. The data were collected at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 80.0 fb$^{-1}$. The $\Upsilon(3S)$ mesons are identified through their dimuon decay channel, while the low-energy photons are detected after converting to e+e- pairs in the silicon tracker, leading to a $\chi_{b}(3P)$ mass resolution of 2.2 MeV. This is the first time that the J=1 and 2 states are well resolved and their masses individually measured: 10513.42$\pm$0.41(stat)$\pm$0.18(syst) MeV and 10524.02$\pm$0.57(stat)$\pm$0.18(syst) MeV; they are determined with respect to the world-average value of the $\Upsilon(3S)$ mass, which has an uncertainty of 0.5 MeV. The mass splitting is measured to be 10.60$\pm$0.64(stat)$\pm$0.17(syst) MeV.
DOI: 10.17182/hepdata.85743.v1/t1
title: "Table 1" of "Observation of the Z $\to\psi\ell^+\ell^-$ decay in pp collisions at $\sqrt{s}=$ 13 TeV"

description: branching fraction ratio of Z-&gt;J/psi+2 leptons over Z-&gt;4muons for the phase space defined above
description: CERN-LHC. Observation of the Z boson decay to a psi meson and two additional leptons using 35.9 fb-1 of pp collisions with CMS. The measurement of the Z-&gt;j/psi+2leptons over the Z-&gt;4muons is also shown.

The Z-&gt;J/psi+2 leptons channel fiducial region is defined as:
- 4mu or 2e2mu
- ptLepton &gt; 30 GeV, ptLepton&gt;15 GeV, ptMuon&gt;3.5GeV, ptMuon&gt;3.5GeV
- 40 &lt; m{non-resonant leptons} &lt; 80 GeV
- |etaElectron| &lt; 2.5
- |etaMuon| &lt; 2.4
- min(DeltaR(l,l)) &gt; 0.2.

The Z-&gt;4 muons channel fiducial region is defined as:
- 4mu or 2e2mu
- ptLepton &gt; 30 GeV, ptLepton&gt;15 GeV, ptMuon&gt;3.5GeV, ptMuon&gt;3.5GeV
- 40 &lt; m{high pt leptons} &lt; 80 GeV
- 4 &lt; m{muons} &lt; 80 GeV
- |etaElectron| &lt; 2.5
- |etaMuon| &lt; 2.4
- min(DeltaR(l,l)) &gt; 0.2.
DOI: 10.17182/hepdata.85744.v1/t1
title: "Table 1" 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 J/psi 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.