cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.3535/y1s-pje-ys2
title: Ennomos fuscantaria (Haworth, 1809)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.156181.v1/t6
title: "Table 6" of "Observation of $\Lambda$ hyperon local polarization in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The second-order Fourier sine coefficients of $\Lambda+\bar{\Lambda}$ polarization along the beam direction as functions of $N_\mathrm{trk}^\mathrm{offline}$ in pPb collisions at 8.16 TeV extracted with HF based event planes. The HF-based event plane is reconstructed only with the HF detectors toward the Pb going direction.
description: No data abstract available.
DOI: 10.17182/hepdata.156182.v1/t1
title: "Table 1" of "Search for medium effects using jet axis decorrelation in inclusive jets from PbPb collisions at $\sqrt{s_\text{NN}}$ = 5.02 TeV"

description: The unfolded jet axis decorrelation distribution,$\frac{1}{N} \frac{dN}{d\Delta j}$, as a function of $\Delta j$ for the $0-10\%$, $10-30\%$, $30-50\%$, and $50-80\%$ centrality bins in the $120 &lt; p_{\mathrm{T}} &lt; 150$ GeV interval.
description: The jet axis decorrelation in inclusive jets is studied using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The jet axis decorrelation is defined as the angular difference between two definitions of the jet axis. It is obtained by applying two recombination schemes on all the constituents of a given jet reconstructed by the anti-$k_{\mathrm{T}}$ sequential algorithm with a distance parameter of $R = 0.4$. The data set, corresponding to an integrated luminosity of $0.662~\mathrm{nb}^{-1}$, was collected in 2018 with the CMS detector at the CERN LHC. The jet axis decorrelations are examined across collision centrality selections and intervals of jet transverse momentum. A centrality dependent evolution of the measured distributions is observed, with a progressive narrowing seen in more central events. This narrowing could result from medium-induced modification of the internal jet structure or reflect color charge effects in energy loss. This new measurement probes jet substructure in previously unexplored kinematic domains and show great promise for providing new insights on the color charge dependence of energy loss to jet-quenching models.
DOI: 10.17182/hepdata.156182.v1/t2
title: "Table 2" of "Search for medium effects using jet axis decorrelation in inclusive jets from PbPb collisions at $\sqrt{s_\text{NN}}$ = 5.02 TeV"

description: The unfolded jet axis decorrelation distribution,$\frac{1}{N} \frac{dN}{d\Delta j}$, as a function of $\Delta j$ for the $0-10\%$, $10-30\%$, $30-50\%$, and $50-80\%$ centrality bins in the $150 &lt; p_{\mathrm{T}} &lt; 190$ GeV interval.
description: The jet axis decorrelation in inclusive jets is studied using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The jet axis decorrelation is defined as the angular difference between two definitions of the jet axis. It is obtained by applying two recombination schemes on all the constituents of a given jet reconstructed by the anti-$k_{\mathrm{T}}$ sequential algorithm with a distance parameter of $R = 0.4$. The data set, corresponding to an integrated luminosity of $0.662~\mathrm{nb}^{-1}$, was collected in 2018 with the CMS detector at the CERN LHC. The jet axis decorrelations are examined across collision centrality selections and intervals of jet transverse momentum. A centrality dependent evolution of the measured distributions is observed, with a progressive narrowing seen in more central events. This narrowing could result from medium-induced modification of the internal jet structure or reflect color charge effects in energy loss. This new measurement probes jet substructure in previously unexplored kinematic domains and show great promise for providing new insights on the color charge dependence of energy loss to jet-quenching models.
DOI: 10.17182/hepdata.156182.v1/t3
title: "Table 3" of "Search for medium effects using jet axis decorrelation in inclusive jets from PbPb collisions at $\sqrt{s_\text{NN}}$ = 5.02 TeV"

description: The unfolded jet axis decorrelation distribution,$\frac{1}{N} \frac{dN}{d\Delta j}$, as a function of $\Delta j$ for the $0-10\%$, $10-30\%$, $30-50\%$, and $50-80\%$ centrality bins in the $190 &lt; p_{\mathrm{T}} &lt; 230$ GeV interval.
description: The jet axis decorrelation in inclusive jets is studied using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The jet axis decorrelation is defined as the angular difference between two definitions of the jet axis. It is obtained by applying two recombination schemes on all the constituents of a given jet reconstructed by the anti-$k_{\mathrm{T}}$ sequential algorithm with a distance parameter of $R = 0.4$. The data set, corresponding to an integrated luminosity of $0.662~\mathrm{nb}^{-1}$, was collected in 2018 with the CMS detector at the CERN LHC. The jet axis decorrelations are examined across collision centrality selections and intervals of jet transverse momentum. A centrality dependent evolution of the measured distributions is observed, with a progressive narrowing seen in more central events. This narrowing could result from medium-induced modification of the internal jet structure or reflect color charge effects in energy loss. This new measurement probes jet substructure in previously unexplored kinematic domains and show great promise for providing new insights on the color charge dependence of energy loss to jet-quenching models.
DOI: 10.17182/hepdata.156182.v1/t4
title: "Table 4" of "Search for medium effects using jet axis decorrelation in inclusive jets from PbPb collisions at $\sqrt{s_\text{NN}}$ = 5.02 TeV"

description: The unfolded jet axis decorrelation distribution,$\frac{1}{N} \frac{dN}{d\Delta j}$, as a function of $\Delta j$ for the $0-10\%$, $10-30\%$, $30-50\%$, and $50-80\%$ centrality bins in the $230 &lt; p_{\mathrm{T}} &lt; 300$ GeV interval.
description: The jet axis decorrelation in inclusive jets is studied using lead-lead (PbPb) collisions at a center-of-mass energy per nucleon pair of 5.02 TeV. The jet axis decorrelation is defined as the angular difference between two definitions of the jet axis. It is obtained by applying two recombination schemes on all the constituents of a given jet reconstructed by the anti-$k_{\mathrm{T}}$ sequential algorithm with a distance parameter of $R = 0.4$. The data set, corresponding to an integrated luminosity of $0.662~\mathrm{nb}^{-1}$, was collected in 2018 with the CMS detector at the CERN LHC. The jet axis decorrelations are examined across collision centrality selections and intervals of jet transverse momentum. A centrality dependent evolution of the measured distributions is observed, with a progressive narrowing seen in more central events. This narrowing could result from medium-induced modification of the internal jet structure or reflect color charge effects in energy loss. This new measurement probes jet substructure in previously unexplored kinematic domains and show great promise for providing new insights on the color charge dependence of energy loss to jet-quenching models.
DOI: 10.3535/k8t-wx3-zf6
title: Cabera pusaria (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/nl8-2vq-ntb
title: Jodis putata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/lgp-04j-m1q
title: Cabera pusaria (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/wfz-j0m-8xa
title: Cabera pusaria (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.131311.v1/t1
title: "Table 1" of "Study of azimuthal anisotropy of $\Upsilon$(1S) mesons in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The $p_{\mathrm{T}}$ dependent $v_{2}^{\textrm{sub}}$ values of $\Upsilon(1S)$ mesons measured in the high-multiplicity region of $70 \leq N^{\text{offline}}_{\text{trk}} &lt; 300$, where a low-multiplicity region of $N^{\text{offline}}_{\text{trk}} &lt; 50$ is used to estimate and correct for the dijet contribution.
description: The azimuthal anisotropy of $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions is studied using data collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The $\mathrm{\Upsilon(1S)}$ mesons are reconstructed using the dimuon decay channel. The anisotropy, characterized by the second Fourier harmonic coefficient $v_2^{\mathrm{sub}}$, is determined using the two-particle correlation technique, in which the $\mathrm{\Upsilon(1S)}$ mesons are correlated with charged hadrons. A large psuedorapidity gap is used to suppress short-range correlations. The $v_2^{\mathrm{sub}}$ values are measured in four transverse momentum intervals in the range from 0 - 30 GeV/c. No azimuthal anisotropy is observed for the $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions, which is consistent with previous PbPb collision results. The results suggest that any collectivity on bottomonia is smaller than that of charmonia in pPb collisions.
DOI: 10.17182/hepdata.131311.v1/t2
title: "Table 2" of "Study of azimuthal anisotropy of $\Upsilon$(1S) mesons in pPb collisions at $\sqrt{s_\mathrm{NN}}$ = 8.16 TeV"

description: The $p_{\mathrm{T}}$ dependent $v_{2}^{\textrm{sub}}$ values of $\Upsilon(1S)$ mesons measured in the high-multiplicity region of $70 \leq N^{\text{offline}}_{\text{trk}} &lt; 300$, where a low-multiplicity region of $N^{\text{offline}}_{\text{trk}} &lt; 50$ is used to estimate and correct for the dijet contribution.
description: The azimuthal anisotropy of $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions is studied using data collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 8.16 TeV. The $\mathrm{\Upsilon(1S)}$ mesons are reconstructed using the dimuon decay channel. The anisotropy, characterized by the second Fourier harmonic coefficient $v_2^{\mathrm{sub}}$, is determined using the two-particle correlation technique, in which the $\mathrm{\Upsilon(1S)}$ mesons are correlated with charged hadrons. A large psuedorapidity gap is used to suppress short-range correlations. The $v_2^{\mathrm{sub}}$ values are measured in four transverse momentum intervals in the range from 0 - 30 GeV/c. No azimuthal anisotropy is observed for the $\mathrm{\Upsilon(1S)}$ mesons in high-multiplicity pPb collisions, which is consistent with previous PbPb collision results. The results suggest that any collectivity on bottomonia is smaller than that of charmonia in pPb collisions.
DOI: 10.3535/fn0-yga-4r6
title: Chlorissa viridata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/hv5-rtj-hhm
title: Cabera pusaria (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/9ac-6n8-qm8
title: Selenia tetralunaria (Hufnagel, 1767)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.135973.v1/t1
title: "Figure 3" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The product of acceptance and efficiency ($A \epsilon$) as a function of $p_{\mathrm{T}}$ for prompt $\Lambda^+_c$ in pp collisions and within centrality regions of 0-90, 0-10, 10-30, 30-50 and 50-90% in PbPb collisions.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.17182/hepdata.135973.v1/t2
title: "Figure 4" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The $p_{\mathrm{T}}$ differential cross sections for prompt $\Lambda^+_c$ production in pp collisions. The global fit uncertainty is 8.6%.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.17182/hepdata.135973.v1/t3
title: "Figure 5" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The $\mathrm{T_{AA}}$-scaled $\Lambda^+_c$ yields as a function of $p_{\mathrm{T}}$ for PbPb collisions within centrality regions of 0-90, 0-10, 10-30, 30-50 and 50-90%.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.17182/hepdata.135973.v1/t4
title: "Figure 6" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The nuclear modification factor $\mathrm{R_{AA}}$ versus $p_{\mathrm{T}}$ for prompt $\Lambda^+_c$ production in centrality regions of 0-90, 0-10, 10-30, 30-50 and 50-90% in PbPb collisions. The global uncertainty includes the uncertainties for the luminosity of pp collisions, number of MB events in PbPb collisions, and tracking efficiency. The global uncertainty for $\mathrm{R_{AA}}$ is 16.5%.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.17182/hepdata.135973.v1/t5
title: "Figure 7 (left)" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The ratio of the production cross sections of prompt $\Lambda^+_c$ to prompt $\mathrm{D_0}$ versus $p_{\mathrm{T}}$ from pp collisions. The global normalization uncertainty is 6.6%.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.17182/hepdata.135973.v1/t6
title: "Figure 7 (right)" of "Study of charm hadronization with prompt $\Lambda^+_\mathrm{c}$ baryons in proton-proton and lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The ratio of the $\mathrm{T_{AA}}$-scaled prompt $\Lambda^+_c$ yields to prompt $\mathrm{D_0}$ versus $p_{\mathrm{T}}$ from PbPb collisions for 0-90 and 0-10% centrality classes. The global normalization uncertainty is 7.3%.
description: The production of prompt $\Lambda_c^+$ baryons is measured via the exclusive decay channel $\Lambda_c^+ \to \mathrm{p} \mathrm{K}^- \pi^+$ at a center-of-mass energy per nucleon pair of $5.02~\mathrm{TeV}$ using $252~\mathrm{nb}^{-1}$ proton-proton (pp) and $0.607~\mathrm{nb}^{-1}$ lead-lead (PbPb) collisions collected at the CERN LHC in 2017 and 2018, respectively. The measurements are performed within the $\Lambda_c^+$ rapidity interval $|y|&lt;1.0$ with transverse momentum ($p_\mathrm{T}$) ranges of 3--30 and 6--40 $\mathrm{GeV}/c$ for pp and PbPb collisions, respectively. Compared to pp collisions scaled by the number of nucleon-nucleon interactions, the observed yields of $\Lambda_c^+$ with $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$ are strongly suppressed in PbPb collisions. The level of suppression depends significantly on both the collision centrality and the $p_\mathrm{T}$ of the $\Lambda_c^+$ baryon. The $\Lambda_c^+/\mathrm{D}^0$ production ratio in PbPb collisions is consistent with the result in pp collisions for $p_\mathrm{T}&gt;10~\mathrm{GeV}/c$, suggesting that the coalescence process of hadronization is not significant for PbPb collisions in the higher $p_\mathrm{T}$ region.
DOI: 10.3535/0r1-pc6-th6
title: Jodis putata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/4zp-ze3-2xp
title: Selenia tetralunaria (Hufnagel, 1767)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/kwg-jd1-byt
title: Chlorissa viridata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/ttn-zqm-6lh
title: Chlorissa viridata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.135972.v1/t1
title: "Table 1" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\eta$ projection of balance function in low $p_{T}$ in 0-10% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.135972.v1/t2
title: "Table 2" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\eta$ projection of balance function in low $p_{T}$ in 30-40% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.135972.v1/t3
title: "Table 3" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\eta$ projection of balance function in low $p_{T}$ in 70-80% centrality
description: No data abstract available.
DOI: 10.17182/hepdata.135972.v1/t4
title: "Table 4" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\phi$ projection of balance function in low $p_{T}$ in 0-10% centrality
description: No data abstract available.
DOI: 10.3535/2ad-naq-bwe
title: Jodis putata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.3535/t2a-sjp-fqa
title: Jodis putata (Linnaeus, 1758)

description: Digital Specimen for the physical specimen hosted at Finnish Museum of Natural History.
DOI: 10.17182/hepdata.135972.v1/t10
title: "Table 10" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\phi$ projection of balance function in low $p_{T}$ in 0-40 $N_{trk}$
description: No data abstract available.
DOI: 10.17182/hepdata.135972.v1/t5
title: "Table 5" of "Multiplicity and transverse momentum dependence of charge-balance functions in pPb and PbPb collisions at LHC energies"

description: $\Delta\phi$ projection of balance function in low $p_{T}$ in 30-40% centrality
description: No data abstract available.