cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.154226.v1/t18
title: "Figure 9.2" of "Investigating strangeness enhancement with multiplicity in pp collisions using angular correlations"

description: $\Xi^{\pm}/\rm K^{0}_{\rm S}$ in pp collisions at $\sqrt{s}=5.02$ TeV, as a function of the charged particle multiplicity measured in events with a trigger particle. Trigger particles are charged particles with $p_\rm{T}&gt;3$ GeV/c.
description: A study of strange hadron production associated with hard scattering processes and with the underlying event is conducted to investigate the origin of the enhanced production of strange hadrons in small collision systems characterised by large charged-particle multiplicities. The production of the single-strange meson ${\rm K}^{0}_{\rm{S}}$ and the double-strange baryon $\Xi^{\pm}$ is measured, in each event, in the azimuthal direction of the highest-$p_{\rm T}$ particle (trigger particle), related to hard scattering processes, and in the direction transverse to it in azimuth, associated with the underlying event, in pp collisions at $\sqrt{s}=5.02$ TeV and $\sqrt{s}=13$ TeV using the ALICE detector at the LHC. The per-trigger yields of ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$ are dominated by the transverse-to-leading production (i.e., in the direction transverse to the trigger particle), whose contribution relative to the toward-leading production is observed to increase with the event charged-particle multiplicity. The transverse-to-leading and the toward-leading $\Xi^{\pm}$/${\rm K}^{0}_{\rm{S}}$ yield ratios increase with the multiplicity of charged particles, suggesting that strangeness enhancement with multiplicity is associated with both hard scattering processes and the underlying event. The relative production of $\Xi^{\pm}$ with respect to ${\rm K}^{0}_{\rm{S}}$ is higher in transverse-to-leading processes over the whole multiplicity interval covered by the measurement. The ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$ per-trigger yields and yield ratios are compared with predictions of three different phenomenological models, namely Pythia8.2 with the Monash tune, Pythia8.2 with ropes and EPOS LHC. The comparison shows that none of them can quantitatively describe either the transverse-to-leading or the toward-leading yields of ${\rm K}^{0}_{\rm{S}}$ and $\Xi^{\pm}$.
DOI: 10.17182/hepdata.154893.v1/t1
title: "Table 1" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $p_{\mathrm{T}}$-differential non-prompt $\mathrm{D}^{0}$ production cross section at midrapidity ($|y|&lt;0.5$) in pp collisions at $\sqrt{s}$ = 13 TeV

Branching ratio of $\mathrm{D}^{0}\rightarrow\mathrm{K}^-\pi^+$: $(3.95 \pm 0.03)\%$.
Global relative uncertainty on BR: $0.8\%$
Global relative uncertainty on luminosity: $1.6\%$
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t2
title: "Table 2" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $p_{\mathrm{T}}$-differential non-prompt $\mathrm{D}^{+}$ production cross section at midrapidity ($|y|&lt;0.5$) in pp collisions at $\sqrt{s}$ = 13 TeV

Branching ratio of $\mathrm{D}^{+}\rightarrow\mathrm{K}^-\pi^+\pi^+$: $(9.38 \pm 0.16)\%$.
Global relative uncertainty on BR: $1.7\%$
Global relative uncertainty on luminosity: $1.6\%$
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t10
title: "Table 10" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $\sigma(\mathrm{D}^{+})$ $\sqrt{s}$ = 13 TeV $/ \sigma(\mathrm{D}^{+})$ $\sqrt{s}$ = 5.02 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t3
title: "Table 3" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $p_{\mathrm{T}}$-differential $\mathrm{D}^{+}_\mathrm{s}$ production cross section at midrapidity ($|y|&lt;0.5$) in pp collisions at $\sqrt{s}$ = 13 TeV

Branching ratio of $\mathrm{D}^{+}_\mathrm{s}\rightarrow\phi\pi^+\rightarrow\mathrm{K}^+\mathrm{K}^-\pi^+$: $(2.22 \pm 0.06)\%$.
Global relative uncertainty on BR: $2.7\%$
Global relative uncertainty on luminosity: $1.6\%$
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t4
title: "Table 4" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: non-prompt / prompt $\sigma(\mathrm{D}^{0})$ $\sqrt{s}$ = 13 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t5
title: "Table 5" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: non-prompt / prompt $\sigma(\mathrm{D}^{+})$ $\sqrt{s}$ = 13 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t6
title: "Table 6" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: non-prompt / prompt $\sigma(\mathrm{D}^{+}_{s})$ $\sqrt{s}$ = 13 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t7
title: "Table 7" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $p_{\mathrm{T}}$-differential non-prompt $\mathrm{D}^{+}/\mathrm{D}^{0}$ ratio in pp collisions at $\sqrt{s}$ = 13 TeV

Global relative uncertainty on BR: $1.9\%$
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t8
title: "Table 8" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $p_{\mathrm{T}}$-differential non-prompt $\mathrm{D}^{+}_\mathrm{s}/(\mathrm{D}^{0}+\mathrm{D}^{+})$ ratio in pp collisions at $\sqrt{s}$ = 13 TeV

Global relative uncertainty on BR: $3.3\%$
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t9
title: "Table 9" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $\sigma(\mathrm{D}^{0})$ $\sqrt{s}$ = 13 TeV / $\sigma(\mathrm{D}^{0})$ $\sqrt{s}$ = 5.02 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.154893.v1/t11
title: "Table 11" of "Measurement of beauty-quark production in pp collisions at $\sqrt{s}=13$ TeV via non-prompt D mesons"

description: $\sigma(\mathrm{D}^{+}_\mathrm{s})$ $\sqrt{s}$ = 13 TeV $/ \sigma(\mathrm{D}^{+}_\mathrm{s})$ $\sqrt{s}$ = 5.02 TeV
description: The $p_{T}$-differential production cross sections of non-prompt $D^{0}$, $D^{+}$, and $D^{+}_{s}$ mesons originating from beauty-hadron decays are measured in proton--proton collisions at a centre-of-mass energy $\sqrt{s}$ of 13 TeV. The measurements are performed at midrapidity, $|y| &lt; 0.5$, with the data sample collected by ALICE from 2016 to 2018. The results are in agreement with predictions from several perturbative QCD calculations. The fragmentation fraction of beauty quarks to strange mesons divided by the one to non-strange mesons, $f_{s}/(f_{u}+f_{d})$, is found to be $0.114 \pm 0.016~{\mathrm (stat.)} \pm 0.006~{\mathrm (syst.)} \pm 0.003~{\mathrm (BR)} \pm 0.003~{\mathrm (extrap.)}$. This value is compatible with previous measurements at lower centre-of-mass energies and in different collision systems in agreement with the assumption of universality of fragmentation functions. In addition, the dependence of the non-prompt D meson production on the centre-of-mass energy is investigated by comparing the results obtained at $\sqrt{s} = 5.02$ and 13~TeV, showing a hardening of the non-prompt D-meson $p_{T}$-differential production cross section at higher $\sqrt{s}$. Finally, the ${\mathrm b\overline{b}}$ production cross section per unit of rapidity at midrapidity is calculated from the non-prompt $D^{0}$, $D^{+}$, $D^{+}_{s}$, and $\Lambda_{c}$ hadron measurements, obtaining $\mathrm{d}\sigma/{\mathrm d}y = 75.2\pm 3.2~(\mathrm{stat.}) \pm 5.2~(\mathrm{syst.})^{+12.3}_{-3.2} ~(\mathrm{extrap.})$$\mu$b
DOI: 10.17182/hepdata.158645.v1/t1
title: "Fig5-data-inclusiveJpsi-assoc0-MB" of "J/$\psi$-hadron correlations at midrapidity in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Near side asociated charged particle yield per trigger in the range $0.15
description: No data abstract available.
DOI: 10.17182/hepdata.158645.v1/t2
title: "Fig5-data-inclusiveJpsi-assoc0-HM" of "J/$\psi$-hadron correlations at midrapidity in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Near side asociated charged particle yield per trigger in the range $0.15
description: No data abstract available.
DOI: 10.17182/hepdata.158645.v1/t3
title: "Fig5-data-promptJpsi-assoc0-MB" of "J/$\psi$-hadron correlations at midrapidity in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Near side asociated charged particle yield per trigger in the range $0.15
description: No data abstract available.
DOI: 10.17182/hepdata.158645.v1/t4
title: "Fig5-data-promptJpsi-assoc0-HM" of "J/$\psi$-hadron correlations at midrapidity in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Near side asociated charged particle yield per trigger in the range $0.15
description: No data abstract available.