cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89268.v1/t24
title: "Table 24" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions as a function of the number of participants for CL1 estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89268.v1/t25
title: "Table 25" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions as a function of the number of participants for V0A estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89268.v1/t26
title: "Table 26" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions as a function of the number of participants for ZNAmult estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89268.v1/t27
title: "Table 27" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions as a function of the number of participants for ZNAPb estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89268.v1/t28
title: "Table 28" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions for 5 participant quarks as a function of the number of participants for CL1 estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.25907/00143
title: Biomass and mineral nutrient partitioning among self-pollinated and cross-pollinated fruit on the same strawberry plant

description: Pollen-parent effects on fruit size and quality have been found previously among competing self-pollinated and cross-pollinated fruit on the same Redlands Joy strawberry plant. These effects occur independently of the percentage of fertilized seeds on the fruit, but the expression of these effects on fruit size and some aspects of quality are greatest when calcium is in shortest supply. Here, we aimed to clarify at what developmental stages the self-pollinated and cross-pollinated fruit diverge in size and quality and whether differences between self-pollinated and cross-pollinated fruit are due to early differences in nutrient accumulation.
DOI: 10.17182/hepdata.89268.v1/t29
title: "Table 29" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Average pseudorapidity density of charged particles in p–Pb NSD collisions for 5 participant quarks as a function of the number of participants for V0A estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89270.v1/t1
title: "Table 1: Results for the ratio of braching fractions" of "Study of the $\mathrm{B}^{+}\rightarrow \mathrm{J}/\psi \bar{\Lambda} \mathrm{p}$ decay in proton-proton collisions at $\sqrt{s}= 8~\mathrm{TeV}$"

description: The measured ratio of branching fractios
description: CERN-LHC-CMS. Study of the B+ to J/psi anti-Lambda p decay in proton-proton collisions at sqrt(s) = 8TeV.
DOI: 10.17182/hepdata.89271.v1/t1
title: "Table 1" of "Observation of a narrow pentaquark state, $P_c(4312)^+$, and of two-peak structure of the $P_c(4450)^+$"

description: Distribution of $(J/\psi p)$ system invariant mass from the decay of $\Lambda_{b}^{0}$ candidates in the channel $\Lambda_{b}^{0} \to J/\psi p K^{-}$.
description: No data abstract available.
DOI: 10.17182/hepdata.89271.v1/t2
title: "Table 2" of "Observation of a narrow pentaquark state, $P_c(4312)^+$, and of two-peak structure of the $P_c(4450)^+$"

description: Distribution of $(J/\psi p)$ system invariant mass from the decay of $\Lambda_{b}^{0}$ candidates in the channel $\Lambda_{b}^{0} \to J/\psi p K^{-}$. $\Lambda_{b}^{0}$ candidates are selected after the suppression of the dominant $\Lambda^{*} \to p K^{-}$ contributions using the $m_{Kp} &gt; 1.9$ GeV$/c^2$ requirement.
description: No data abstract available.
DOI: 10.17182/hepdata.89271.v1/t3
title: "Table 3" of "Observation of a narrow pentaquark state, $P_c(4312)^+$, and of two-peak structure of the $P_c(4450)^+$"

description: $\cos \theta_{P_c}$-weighted ditribution of $(J/\psi p)$ system invariant mass from the decay of $\Lambda_{b}^{0}$ candidates in the channel $\Lambda_{b}^{0} \to J/\psi p K^{-}$. Here $\theta_{P_c}$ is the helicity angle of the pentaquark exotic state (the angle between $K^-$ and $J/\psi$ in the pentaquark state rest frame).
description: No data abstract available.
DOI: 10.17182/hepdata.89271.v1/t4
title: "Table 4" of "Observation of a narrow pentaquark state, $P_c(4312)^+$, and of two-peak structure of the $P_c(4450)^+$"

description: Spline interpolation of the weight function (depending of $\cos \theta_{P_c}$) applied to $\Lambda_{b}^{0}$ candidates. The weight function is determined as the inverse of the density of $\Lambda_{b}^{0}$ candidates in the narrow pentaquark peak region while the interpolation is done between the bin centers.
description: No data abstract available.
DOI: 10.17182/hepdata.89272.v1/t1
title: "Table 2" of "Centrality dependence of charged-particle pseudorapidity distributions from d + Au collisions at s(NN)**(1/2) = 200-GeV."

description: $\frac{\mathrm{d}N}{\mathrm{d}\eta}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{d}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$ for $0-30$% central, $30-60$% central, $60-80$% central, Min.Bias
description: BNL-RHIC-BRAHMS. Charged-particle pseudorapidity densities are presented for the d+Au reaction at sqrt{s_{NN}}=200 GeV with -4.2 &lt;= eta &lt;= 4.2$. The results, from the BRAHMS experiment at RHIC, are shown for minimum-bias events and 0-30%, 30-60%, and 60-80% centrality classes. Models incorporating both soft physics and hard, perturbative QCD-based scattering physics agree well with the experimental results. The data do not support predictions based on strong-coupling, semi-classical QCD. In the deuteron-fragmentation region the central 200 GeV data show behavior similar to full-overlap d+Au results at sqrt{s_{NN}}=19.4 GeV.
DOI: 10.5281/zenodo.17525513
title: Observation of a phonon bottleneck effect on the thermal depopulation from a photoexcited shallow defect in silicon

description: Main results collected in the published article Revuelta, S., et. al. Observation of a phonon bottleneck effect on the thermal depopulation from a phoexcited shallow defect in silicon. Phys. Rev. B - Accepted 28.10.2025, DOI: https://doi.org/10.1103/5mpm-zc9s
DOI: 10.5281/zenodo.17525514
title: Observation of a phonon bottleneck effect on the thermal depopulation from a photoexcited shallow defect in silicon

description: Main results collected in the published article Revuelta, S., et. al. Observation of a phonon bottleneck effect on the thermal depopulation from a phoexcited shallow defect in silicon. Phys. Rev. B - Accepted 28.10.2025, DOI: https://doi.org/10.1103/5mpm-zc9s
DOI: 10.17182/hepdata.89268.v1/t12
title: "Table 12" of "Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV"

description: Pseudorapidity density of charged particles in p–Pb NSD collisions at 8.16 TeV for 10-20% centrality class and V0A estimator.
description: Measurements of charged particle multiplicity density in p-Pb collisions at centre-of-mass energies of 8.16 TeV in the pseudorapidity range -1.7 to 1.7. Results are given for NSD (non-single diffractive, i.e. non-diffractive and double processes only) class of events and for different centrality estimators, CL1 (mid-rapidity multiplicity estimator), V0A (forward-rapidity multiplicity estimator) and ZNA (energy deposited in the Zero Degree Calorimeter).
DOI: 10.17182/hepdata.89304.v1/t1
title: "Table 1" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-p collisions at 7 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t2
title: "Table 2" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-p collisions at 7 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t3
title: "Table 3" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-p collisions at 7 TeV with 0.6
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t4
title: "Table 4" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-p collisions at 7 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t5
title: "Table 5" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-p collisions at 7 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t10
title: "Table 10" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-Pb collisions at 5.02 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t11
title: "Table 11" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-Pb collisions at 5.02 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t12
title: "Table 12" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-Pb collisions at 5.02 TeV with 0.6
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t6
title: "Table 6" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for wide component in p-p collisions at 7 TeV with 0.6
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t7
title: "Table 7" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-Pb collisions at 5.02 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t8
title: "Table 8" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-Pb collisions at 5.02 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t9
title: "Table 9" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables RMS for narrow component in p-Pb collisions at 5.02 TeV with 0.6
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t13
title: "Table 13" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables per-trigger yield for narrow component in p-p collisions at 7 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t14
title: "Table 14" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables per-trigger yield for narrow component in p-p collisions at 7 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t15
title: "Table 15" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables per-trigger yield for narrow component in p-p collisions at 7 TeV with 0.6
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t16
title: "Table 16" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables per-trigger yield for wide component in p-p collisions at 7 TeV with 0.2
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.
DOI: 10.17182/hepdata.89304.v1/t17
title: "Table 17" of "Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions"

description: trigger particle momentum dependence of observables per-trigger yield for wide component in p-p collisions at 7 TeV with 0.4
description: CERN-LHC. The transverse structure of jets was studied via jet fragmentation transverse momentum ($j_{\rm T}$) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region $3 &lt; p_{\rm T} &lt; 15$ ~GeV/$c$ is explored in this study.