cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.135833.v3/t1
title: "Figure 2" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The jet multiplicity for $N_\textrm{b} \geq 4$ in the opposite-sign dilepton channel for the combined 2017--2018 dataset with dilepton decay categories combined. Here, $\textrm{t}\bar{\textrm{t}} + \geq 1 \textrm{b}$ refers to $\textrm{t}\bar{\textrm{t}}$ events with at least one additional b jet, $\textrm{t}\bar{\textrm{t}} + 0 \textrm{b}$ includes all other $\textrm{t}\bar{\textrm{t}}$ events not produced in association with a boson, and EW refers to events that contain W and Z bosons but no top quarks. The backgrounds and $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal (derived from the fit) are shown as a stacked histogram. The hatched bands correspond to the estimated total uncertainty after the fit.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t2
title: "Figure 3" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the 2016--2018 data set for three different categories in the combined single-electron and single-muon channels. The three categories are defined by the number of resolved t tags ($N_\textrm{RT}$), b tags ($N_\textrm{b}$), and jets ($N_\textrm{j}$), selected as representative based on their sensitivity to signal. Here, $\textrm{t}\bar{\textrm{t}} + \geq 1 \textrm{b}$ refers to $\textrm{t}\bar{\textrm{t}}$ events with at least one additional b jet, while $\textrm{t}\bar{\textrm{t}} + 0 \textrm{b}$ includes all other $\textrm{t}\bar{\textrm{t}}$ events not produced in association with a boson. The TOP grouping contains single top quark production along with the other $\textrm{t}\bar{\textrm{t}}$ processes not explicitly shown, and EW refers to events that contain W and Z bosons but no top quarks. The backgrounds and $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal (derived from the fit) are shown as a stacked histogram. The hatched bands correspond to the estimated total uncertainty after the fit. While the bins are shown to be equal width, they do not correspond to equal width in BDT value.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t3
title: "Figure 4a" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The sample VR category shown is defined by $N_\textrm{RT}=1$, $N_\textrm{BT} \geq 1$, $H_T &gt; 1400$ GeV. The background from QCD multijet and $\textrm{t}\bar{\textrm{t}}$ production is derived from control regions in the data. Estimates for the $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal and other backgrounds are shown using simulated samples. The hatched bands correspond to the estimated total uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t4
title: "Figure 4b" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The sample VR category shown is defined by $N_\textrm{RT} \geq 2$, $H_T &gt; 1100$ GeV. The background from QCD multijet and $\textrm{t}\bar{\textrm{t}}$ production is derived from control regions in the data. Estimates for the $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal and other backgrounds are shown using simulated samples. The hatched bands correspond to the estimated total uncertainty.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t5
title: "Figure 6a" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The SR category shown in this figure is defined by $N_\textrm{RT}=1$, $N_\textrm{BT} \geq 1$, $H_T &gt; 1400$ GeV. The background from QCD multijet and $\textrm{t}\bar{\textrm{t}}$ production is derived from control regions in the data. Estimates for the $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal and other backgrounds are shown using simulated samples. The hatched bands correspond to the estimated total uncertainty after the fit.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t6
title: "Figure 6b" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The SR category shown in this figure is defined by $N_\textrm{RT} = 2$, $H_T &gt; 1100$ GeV. The background from QCD multijet and $\textrm{t}\bar{\textrm{t}}$ production is derived from control regions in the data. Estimates for the $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ signal and other backgrounds are shown using simulated samples. The hatched bands correspond to the estimated total uncertainty after the fit.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t7
title: "Figure 7" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed significance (in standard deviations) for $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ production from each final state and the combination with previous CMS results (EPJC 80 (2020) 75 and JHEP 11 (2019) 082). The same-sign dilepton and multilepton (SSDL\&ML) final state results are from EPJC 80 (2020) 75.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t1
title: "Figure 2" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The jet multiplicity for $N_\textrm{b} \ge 4$ in the opposite-sign dilepton channel for the combined 2017--2018 dataset with dilepton decay categories combined. Here, $\textrm{t}\bar{\textrm{t}} + \geq 1 \textrm{b}$ refers to $\textrm{t}\bar{\textrm{t}}$ events with at least one additional b jet, $\textrm{t}\bar{\textrm{t}} + 0 \textrm{b}$ includes all other $\textrm{t}\bar{\textrm{t}}$ events not produced in association with a boson, and EW refers to events that contain W and Z bosons but no top quarks.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t2
title: "Figure 3" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the 2016--2018 data set for three different categories in the combined single-electron and single-muon channels. The three categories are defined by the number of resolved t tags ($N_\textrm{RT}$), b tags ($N_\textrm{b}$), and jets ($N_\textrm{j}$), selected as representative based on their sensitivity to signal. Here, $\textrm{t}\bar{\textrm{t}} + \geq 1 \textrm{b}$ refers to $\textrm{t}\bar{\textrm{t}}$ events with at least one additional b jet, while $\textrm{t}\bar{\textrm{t}} + 0 \textrm{b}$ includes all other $\textrm{t}\bar{\textrm{t}}$ events not produced in association with a boson. The TOP grouping contains single top quark production along with the other $\textrm{t}\bar{\textrm{t}}$ processes not explicitly shown, and EW refers to events that contain W and Z bosons but no top quarks.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t3
title: "Figure 5a" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The SR category shown in this figure is defined by $N_\textrm{RT}=1$, $N_\textrm{BT} \geq 1$, HT &gt; 1400 GeV. The background from QCD multijet and \ttbar production is derived from control regions in the data. Estimates for the \tttt signal and other backgrounds are shown using simulated samples.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t4
title: "Figure 5b" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distribution of the BDT discriminants for the full 2016--2018 data set in the all-hadronic channel. The SR category shown in this figure is defined by $N_\textrm{BT} \geq 2$, HT &gt; 1100 GeV. The background from QCD multijet and \ttbar production is derived from control regions in the data. Estimates for the \tttt signal and other backgrounds are shown using simulated samples.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v3/t8
title: "Table 2" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured signal strength ($\mu = \sigma_{\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}}/ \sigma_{\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}} ^{\textrm{SM}}$), corresponding cross section (in fb), and the expected and observed significance (in standard deviations) for $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ production from all analysis channels. This table shows production from each analysis channel in this Letter, the combination of those channels, the results from previously published results, and the full combination of all CMS 2016-2018 results.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t5
title: "Figure 6" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed significance (in standard deviations) for $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ production from each final state and the combination with previous CMS results (EPJC 80 (2020) 75 and JHEP 11 (2019) 082). The same-sign dilepton and multilepton (SSDL\&ML) final state results are from EPJC 80 (2020) 75.
description: No data abstract available.
DOI: 10.17182/hepdata.135833.v1/t6
title: "Table 1" of "Evidence for four-top quark production in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured signal strength ($\mu = \sigma_{\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}}/ \sigma_{\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}} ^{\textrm{SM}}$), corresponding cross section (in fb), and the expected and observed significance (in standard deviations) for $\textrm{t}\bar{\textrm{t}}\textrm{t}\bar{\textrm{t}}$ production from all analysis channels. Uncertainties shown in this table are statistical and systematic uncertainties respectively. In this table, SSDL\&ML and OSDL (2016) represent results from EPJC 80 (2020) 75 and JHEP 11 (2019) 082 respectively.
description: No data abstract available.
DOI: 10.15468/dl.f9pazn
title: Occurrence Download

description: A dataset containing 1346 species occurrences available in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is Human Observation",
 "DatasetKey is iNaturalist Research-grade Observations",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Larix lyallii",
 "Year 2020-2025"
 ]
}

 The dataset includes 1346 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015985-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.135974.v1/t1
title: "Table 1-1" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the integrated three-particle correlators for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t2
title: "Table 1-2" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the integrated three-particle correlators for Au+Au collisions at 39.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t3
title: "Table 1-3" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the integrated three-particle correlators for Au+Au collisions at 27.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t4
title: "Table 2-1" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the inclusive, mode-coupled and linear higher-order flow harmonics $v_4$ for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t5
title: "Table 2-2" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the inclusive, mode-coupled and linear higher-order flow harmonics $v_5$ for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t6
title: "Table 2-3" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the inclusive, mode-coupled and linear higher-order flow harmonics $v_4$ for Au+Au collisions at 39.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t7
title: "Table 2-4" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the inclusive, mode-coupled and linear higher-order flow harmonics $v_4$ for Au+Au collisions at 27.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t10
title: "Table 3-3" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $\chi_{4,22}$ and $\rho_{4,22}$ for Au+Au collisions at 39.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t11
title: "Table 3-4" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $\chi_{4,22}$ and $\rho_{4,22}$ for Au+Au collisions at 27.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t12
title: "Table 4-1" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $NSC(2,3)$ and $NSC(2,4)$ for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t13
title: "Table 4-2" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $NSC(2,3)$ and $NSC(2,4)$ for Au+Au collisions at 27.0 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t8
title: "Table 3-1" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $\chi_{4,22}$ and $\rho_{4,22}$ for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135974.v1/t9
title: "Table 3-2" of "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions"

description: Comparison of the $\chi_{3,23}$ and $\rho_{5,23}$ for Au+Au collisions at 54.4 GeV.
description: "Beam energy dependence of the linear and mode-coupled flow harmonics in Au+Au collisions."
DOI: 10.17182/hepdata.135986.v1/t1
title: "Table 0" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Production yield of non-prompt $\mathrm{D}_{s}^{\pm}$ candidates average for 0-10% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t2
title: "Table 1" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Production yield of non-prompt $\mathrm{D}_{s}^{\pm}$ candidates average for 30-50% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t11
title: "Table 10" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt $\mathrm{D}_{s}^{+}$ over non-prompt $\mathrm{D}^{0}$ Raa in 30-50% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t3
title: "Table 2" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Yield ratio of non-prompt over prompt $\mathrm{D}_{s}^{+}$ for 0-10% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t4
title: "Table 3" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Yield ratio of non-prompt over prompt $\mathrm{D}_{s}^{+}$ for 30-50% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t5
title: "Table 4" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Yield ratio of non-prompt $\mathrm{D}_{s}^{+}$ over non-prompt $\mathrm{D}^{0}$ for pp collisions at $\sqrt{s} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t6
title: "Table 5" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Yield ratio of non-prompt $\mathrm{D}_{s}^{+}$ over non-prompt $\mathrm{D}^{0}$ for 0-10% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t7
title: "Table 6" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Yield ratio of non-prompt $\mathrm{D}_{s}^{+}$ over non-prompt $\mathrm{D}^{0}$ for 30-50% Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4
DOI: 10.17182/hepdata.135986.v1/t8
title: "Table 7" of "Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons"

description: Non-prompt $\mathrm{D}_{s}^{+}$ Raa in 0-10% collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.
description: The production yields of non-prompt $\mathrm{D}_{s}^{+}$ mesons, namely $\mathrm{D}_{s}^{+}$ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum ($p_{T}$) at midrapidity ($|y|&lt;0.5$) in central and semi-central Pb--Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=5.02~$TeV with the ALICE experiment at the LHC.The $\mathrm{D}_{s}^{\pm}$ mesons were reconstructed from the hadronic decay channel $\rm D_s^{+}\to \phi\pi^+$, with $\rm \phi\to K^-K^+$, in the $4