cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.156190.v1/t9
title: "Table 9 - Antiproton PT spectrum rapidity 0.1 to 0.2" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.1 to 0.2.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t11
title: "Table 11 - Antiproton PT spectrum rapidity 0.3 to 0.4" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.3 to 0.4.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t12
title: "Table 12 - Antiproton PT spectrum rapidity 0.4 to 0.5" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.4 to 0.5.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t13
title: "Table 13 - Antiproton PT spectrum rapidity 0.5 to 0.6" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.5 to 0.6.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t14
title: "Table 14 - Antiproton PT spectrum rapidity 0.6 to 0.7" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Transverse momentum spectra of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as shown in Fig. 1 (left panel). Rapidity interval 0.6 to 0.7.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t15
title: "Table 15 - Antideuteron integrated yields vs rapidity" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Integrated yields of antideuterons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of absolute value of rapidity. The figure is shown in Fig. 2 (right panel).
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t16
title: "Table 16 - Antiproton integrated yields vs rapidity" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: Integrated yields of antiprotons measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of absolute value of rapidity. The figure is shown in Fig. 2 (left panel).
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t17
title: "Table 17 - B2 vs PT per nucleon rapidity 0.0 to 0.1" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.0 to 0.1, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t18
title: "Table 18 - B2 vs PT per nucleon rapidity 0.1 to 0.2" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.1 to 0.2, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t19
title: "Table 19 - B2 vs PT per nucleon rapidity 0.2 to 0.3" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.2 to 0.3, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t20
title: "Table 20 - B2 vs PT per nucleon rapidity 0.3 to 0.4" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.3 to 0.4, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t21
title: "Table 21 - B2 vs PT per nucleon rapidity 0.4 to 0.5" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.4 to 0.5, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t22
title: "Table 22 - B2 vs PT per nucleon rapidity 0.5 to 0.6" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.5 to 0.6, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t23
title: "Table 23 - B2 vs PT per nucleon rapidity 0.6 to 0.7" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of transverse momentum per nucleon. The figure is shown in Fig. 3, rapidity interval 0.6 to 0.7, in absolute value.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t24
title: "Table 24 - B2 vs Y for PToverA 0.9 to 1.0" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of rapidity, for fixed intervals of transverse momentum per nucleon. The data is shown in Fig. 4, in the PT per nucleon interval from 0.9 to 1.0.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t25
title: "Table 25 - B2 vs Y for PToverA 1.0 to 1.1" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of rapidity, for fixed intervals of transverse momentum per nucleon. The data is shown in Fig. 4, in the PT per nucleon interval from 1.0 to 1.1.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t26
title: "Table 26 - B2 vs Y for PToverA 1.1 to 1.3" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of rapidity, for fixed intervals of transverse momentum per nucleon. The data is shown in Fig. 4, in the PT per nucleon interval from 1.1 to 1.3.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.151390.v1/t1
title: "Table 1" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse momentum spectra in different multiplicity classes. Each spectrum is corrected for the branching ratio of (46 $\pm$ 6)% based on [Phys. Rev. Lett. 111 no. 6, (2013) 062001].
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.151390.v1/t2
title: "Table 2" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The ratio of transverse momentum spectrum to the NSD spectrum
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.151390.v1/t3
title: "Table 3" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The double ratio of particle yield of f0((980) to charged pions
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.151390.v1/t4
title: "Table 4" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: The double ratio of particle yield of f0((980) to K*(892)0
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.151390.v1/t5
title: "Table 5" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse-momentum-differential particle yield ratio of f$_{0}$(980) to charged pions and its double ratio
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.151390.v1/t6
title: "Table 6" of "Observation of abnormal suppression of $\mathrm{f}_{0}$(980) production in p$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Transverse-momentum-differential particle yield ratio of f$_{0}$(980) to K$^{*}(892)$^{0}$ and its double ratio
description: The dependence of f$_{0}$(980) production on the final-state charged-particle multiplicity in p-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is reported. The production of f$_{0}$(980) is measured with the ALICE detector via the f$_{0}$(980) $\rightarrow \pi^{+}\pi^{-}$ decay channel in a midrapidity region of $-0.5 &lt; \mathrm{y} &lt; 0$. Particle yield ratios of f$_{0}$(980) to $\pi$ and K$^{*}$(892)$^{0}$ are found to be decreasing with increasing charged-particle multiplicity. The magnitude of the suppression of the f$_{0}$(980)/$\pi$ and f$_{0}$(980)/K$^{*}$(892)$^{0}$ yield ratios is found to be dependent on the transverse momentum $p_\mathrm{T}$, suggesting different mechanisms responsible for the measured effects. Furthermore, the nuclear modification factor $Q_\mathrm{pPb}$ of f$_{0}$(980) is measured in various multiplicity ranges. The $Q_\mathrm{pPb}$ shows a strong suppression of the f$_{0}$(980) production in the $p_\mathrm{T}$ region up to about 4 GeV/$c$ The results on the particle yield ratios and $Q_\mathrm{pPb}$ for f$_{0}$(980) may help to understand the late hadronic phase in p-Pb collisions and the nature of the internal structure of f$_{0}$(980) particle
DOI: 10.17182/hepdata.156190.v1/t27
title: "Table 27 - B2 vs Y for PToverA 1.3 to 1.5" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of rapidity, for fixed intervals of transverse momentum per nucleon. The data is shown in Fig. 4, in the PT per nucleon interval from 1.3 to 1.5.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.
DOI: 10.17182/hepdata.156190.v1/t28
title: "Table 28 - B2 vs Y for PToverA 1.5 to 1.7" of "Rapidity dependence of antideuteron coalescence in pp collisions at $\sqrt{s}$ = 13 TeV with ALICE"

description: coalescence parameter B2 measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, as a function of rapidity, for fixed intervals of transverse momentum per nucleon. The data is shown in Fig. 4, in the PT per nucleon interval from 1.5 to 1.7.
description: Transverse momentum spectra of antideuterons as a function of rapidity, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV, are shown in Fig. 1. The coalescence parameters B2 as a function of the transverse momentum per nucleon are reported in Fig. 2.