cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.129148.v1/t11
title: "Table 11" of "Measurement of K$^{*}$(892)$^{\mathrm{\pm}}$ production in inelastic pp collisions at the LHC"

description: The p$_{T}$ integrated (K*(892)$^{+}$+ K*(892)$^{-}$)/2 in the interval
 0
description: CERN-LHC. The first results on K*(892)$^{\pm}$ resonance production in inelastic pp collisions at LHC energies of $\sqrt{s}$ = 5.02, 8, and 13 TeV are reported. The K*(892)$^{\pm}$ has been reconstructed via its hadronic decay channel K*(892)$^{\pm} \rightarrow$ $\mathrm {K^0_S}$ $~+~\pi^{\pm}$ with the ALICE detector. Transverse momentum distributions measured at mid-rapidity, integrated yields, and mean transverse momenta are presented.
The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at $\sqrt{s}$ = 5.02, 8 and 13 TeV to the K*(892)$^{0}$ spectrum at the same collision energy is reported. The ratio of each measured p$_{T}$ distribution for K*(892)$^{\pm}$ mesons at
$\sqrt{s}$ = 5.02 and 13 TeV to the K spectrum at the same collision energy is also reported. The pp data at $\sqrt{s}$ = 5.02 and 13 TeV were collected in 2015 while data at $\sqrt{s}$ = 8 TeV were collected in 2012, with integrated luminosities of 2.12, 0.92 and 1.25 nb$^{-1}$, respectively.
DOI: 10.17182/hepdata.159928.v1/t1
title: "Figure 2 left" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Resolutions of the first-order event plane from the ZDC-SMDs as a function of collision centrality in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t2
title: "Figure 2 right" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Resolutions of the second-order event plane from the TPC as a function of collision centrality in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t3
title: "Figure 3 left panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference as a function of centrality in combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t4
title: "Figure 3 right panel Ru+Ru" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Ru+Ru collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t5
title: "Figure 3 right panel Zr+Zr" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t11
title: "Figure 6" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The pseudorapidity dependence of $\Lambda$+$\bar\Lambda$ $P_{\rm H}$ for 20\%-60\% centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV, together with the results for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t6
title: "Figure 3 right panel Ru+Ru&Zr+Zr" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$ and $\bar\Lambda$ and their difference in 20-50\% centrality in Ru+Ru&Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t7
title: "Figure 4 centrality left panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$+$\bar\Lambda$ as a function of centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV (left panel). The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t8
title: "Figure 4 centrality right panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$+$\bar\Lambda$ in 20-50\% centrality centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV (right panel). The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t9
title: "Figure 4 npart" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Lambda$+$\bar\Lambda$ as a function of the average number of participants $\langle N_{\rm part} \rangle$ in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.
description: No data abstract available.
DOI: 10.6084/m9.figshare.30702265
title: Plant Species Composition, Richness, and Diversity in Areas Invaded by Non-Native Plants in the Lower Montane Forest of Kilimanjaro National Park, Tanzania

description: The present study assessed the impact of invasive alien species on plant species composition, richness, and diversity in the lower montane forest of Kilimanjaro National Park. The study area was categorized into four sites: the first three dominated by non-native species, namely Black Wattle (<i>Acacia mearnsii</i>), Mexican weeping pine (<i>Pinus patula</i>), and Eucalyptus (<i>Eucalyptus</i> spp.), and the fourth zone comprised natural forests. Sixty plots, each measuring 20 m × 50 m, were established at each site for vegetation sampling. A total of 168 plant species representing 135 genera and 64 families were identified and recorded from the study area. The highest plant species diversity was recorded in the natural forest with a mean plant species number of 13.8 ± 1.7, followed by <i>Eucalyptus</i> spp. <i>A. mearnsii</i>, and <i>P. patula</i> with 10.3 ± 1.2, 10.13 ± 1.1, and 7.33 ± 1.1, respectively. The plant species richness was significantly higher in the natural forest than in the areas invaded with non-native plant species (<i>p</i> &lt; .05). Natural forest had the highest tree density of native trees with 774 ± 111 stems/ha and the lowest was observed in the <i>P. patula</i> site with a mean density of 12.7 ± 6.9. The reduction in plant species diversity and density in areas invaded with invasive alien species highlights the negative impact these species have on native plant communities. Sustainable forest management focusing on the protection of natural forests, the control of invasive species, and forest enrichment is highly recommended.
DOI: 10.6084/m9.figshare.30702265.v1
title: Plant Species Composition, Richness, and Diversity in Areas Invaded by Non-Native Plants in the Lower Montane Forest of Kilimanjaro National Park, Tanzania

description: The present study assessed the impact of invasive alien species on plant species composition, richness, and diversity in the lower montane forest of Kilimanjaro National Park. The study area was categorized into four sites: the first three dominated by non-native species, namely Black Wattle (<i>Acacia mearnsii</i>), Mexican weeping pine (<i>Pinus patula</i>), and Eucalyptus (<i>Eucalyptus</i> spp.), and the fourth zone comprised natural forests. Sixty plots, each measuring 20 m × 50 m, were established at each site for vegetation sampling. A total of 168 plant species representing 135 genera and 64 families were identified and recorded from the study area. The highest plant species diversity was recorded in the natural forest with a mean plant species number of 13.8 ± 1.7, followed by <i>Eucalyptus</i> spp. <i>A. mearnsii</i>, and <i>P. patula</i> with 10.3 ± 1.2, 10.13 ± 1.1, and 7.33 ± 1.1, respectively. The plant species richness was significantly higher in the natural forest than in the areas invaded with non-native plant species (<i>p</i> &lt; .05). Natural forest had the highest tree density of native trees with 774 ± 111 stems/ha and the lowest was observed in the <i>P. patula</i> site with a mean density of 12.7 ± 6.9. The reduction in plant species diversity and density in areas invaded with invasive alien species highlights the negative impact these species have on native plant communities. Sustainable forest management focusing on the protection of natural forests, the control of invasive species, and forest enrichment is highly recommended.
DOI: 10.17182/hepdata.159928.v1/t10
title: "Figure 5" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The transverse momentum dependence of $\Lambda$+$\bar\Lambda$ $P_{\rm H}$ for 20\%-60\% centrality in the combined Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV, together with the results for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data in Au+Au collisions is from Phys. Rev. C 98 (2018) 014910.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t12
title: "Figure 7 left panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The polarization coefficient $P_{y,c0}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 as a function of centrality (left panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ is same data as in Figure 4.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t13
title: "Figure 7 right panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The polarization coefficient $P_{y,c0}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 for 20-50\% centrality (right panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ is same data as in Figure 4.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t14
title: "Figure 8 left panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The polarization coefficient $P_{y,c2}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 as a function of centrality (left panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.6084/m9.figshare.30702267
title: Epidemiological characteristics and temporal trends of male infertility in Egypt (2012–2022): Analysis of 3,037 consecutive cases

description: Male factors contribute to about half of global infertility cases, yet regional data are limited, particularly in Egypt. To characterize the sociodemographic, clinical, seminal, and hormonal profiles of infertile Egyptian men and investigate their correlations. We retrospectively analyzed the medical records of infertile men presented to a single busy andrology/infertility center in Egypt between June 2012 and May 2022. Demographic, clinical, seminal, and hormonal data were reviewed, and trends and correlations were assessed. Of 3,037 men, primary infertility accounted for 76.13%, with a median infertility duration of 4 years. Varicocele was observed in 66.47% of cases, predominantly second-degree. Asthenozoospermia (31.74%), oligoasthenozoospermia (20.78%), and azoospermia (9.12%) were the most frequent semen abnormalities. Median sperm concentration was 24 million/ml, progressive motility 25%, and normal morphology 10%. From 2012 to 2022, median sperm concentration declined from 24 million/ml to 18 million/ml (<i>p</i> = 0.2), progressive motility declined from 25% to 17% (<i>p</i> &lt; 0.001), and normal sperm morphology declined from 10% to 5% (<i>p</i> &lt; 0.001). The COVID-19 pandemic period (2020–2022) exhibited the most prominent reduction in sperm progressive motility (from 21% to 17%; <i>p</i> &lt; 0.001). Smoking negatively correlated with all sperm parameters. Follicle-stimulating hormone and luteinizing hormone levels correlated negatively with semen quality and testicular volume but positively with infertility duration. Neither varicocele grade nor total testosterone levels correlated significantly with sperm parameters. This study identified primary infertility, varicocele diagnosis and asthenozoospermia as predominant findings among infertile Egyptian men. Over a decade, temporal declines in sperm concentration, motility, and morphology were observed, exacerbated by the COVID-19 pandemic. Smoking and elevated gonadotropins negatively influenced semen quality and testicular volume, whereas testosterone levels and varicocele grade showed no significant correlation. These findings highlight the importance of developing integrated, region-specific strategies to address male infertility.
DOI: 10.6084/m9.figshare.30702267.v1
title: Epidemiological characteristics and temporal trends of male infertility in Egypt (2012–2022): Analysis of 3,037 consecutive cases

description: Male factors contribute to about half of global infertility cases, yet regional data are limited, particularly in Egypt. To characterize the sociodemographic, clinical, seminal, and hormonal profiles of infertile Egyptian men and investigate their correlations. We retrospectively analyzed the medical records of infertile men presented to a single busy andrology/infertility center in Egypt between June 2012 and May 2022. Demographic, clinical, seminal, and hormonal data were reviewed, and trends and correlations were assessed. Of 3,037 men, primary infertility accounted for 76.13%, with a median infertility duration of 4 years. Varicocele was observed in 66.47% of cases, predominantly second-degree. Asthenozoospermia (31.74%), oligoasthenozoospermia (20.78%), and azoospermia (9.12%) were the most frequent semen abnormalities. Median sperm concentration was 24 million/ml, progressive motility 25%, and normal morphology 10%. From 2012 to 2022, median sperm concentration declined from 24 million/ml to 18 million/ml (<i>p</i> = 0.2), progressive motility declined from 25% to 17% (<i>p</i> &lt; 0.001), and normal sperm morphology declined from 10% to 5% (<i>p</i> &lt; 0.001). The COVID-19 pandemic period (2020–2022) exhibited the most prominent reduction in sperm progressive motility (from 21% to 17%; <i>p</i> &lt; 0.001). Smoking negatively correlated with all sperm parameters. Follicle-stimulating hormone and luteinizing hormone levels correlated negatively with semen quality and testicular volume but positively with infertility duration. Neither varicocele grade nor total testosterone levels correlated significantly with sperm parameters. This study identified primary infertility, varicocele diagnosis and asthenozoospermia as predominant findings among infertile Egyptian men. Over a decade, temporal declines in sperm concentration, motility, and morphology were observed, exacerbated by the COVID-19 pandemic. Smoking and elevated gonadotropins negatively influenced semen quality and testicular volume, whereas testosterone levels and varicocele grade showed no significant correlation. These findings highlight the importance of developing integrated, region-specific strategies to address male infertility.
DOI: 10.17182/hepdata.140098.v1/t2
title: "Table 2" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 10-20% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t3
title: "Table 3" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 20-30% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t4
title: "Table 4" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 30-40% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t15
title: "Figure 8 right panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: The polarization coefficient $P_{y,c2}$ of $\Lambda\!+\!\bar\Lambda$ from method-1 and method-2 for 20-50\% centrality (right panel) in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t16
title: "Figure 9 left panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Xi^{-}$+$\bar\Xi^{+}$ from polarization transfer method and direct measurement method as a function of centrality (left panel) in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV. In this figure, $P_{H}$ of inclusive $\Lambda+\bar\Lambda$ is same data as in Figure 4.
description: No data abstract available.
DOI: 10.17182/hepdata.159928.v1/t17
title: "Figure 9 right panel" of "Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV"

description: Global polarization of $\Xi^{-}$+$\bar\Xi^{+}$ from polarization transfer method and direct measurement method for 20-50\% centrality (right panel) in Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV . In this figure, $P_{H}$ of inclusive $\Lambda+\bar\Lambda$ is same data as in Figure 4.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t1
title: "Table 1" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 0-10% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t5
title: "Table 5" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 40-50% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t6
title: "Table 6" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 50-60% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t7
title: "Table 7" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 60-70% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t10
title: "Table 10" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 40-60% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t11
title: "Table 11" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 60-80% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t13
title: "Table 13" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 10-20% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t8
title: "Table 8" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 70-80% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t9
title: "Table 9" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in 20-40% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t12
title: "Table 12" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 0-10% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t14
title: "Table 14" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 20-30% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t15
title: "Table 15" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 30-40% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t16
title: "Table 16" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 40-50% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t17
title: "Table 17" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 50-60% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.140098.v1/t18
title: "Table 18" of "Production of K$^{*}(892)^{0}$ and $\phi(1020)$ in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: $p_{T}$-dependent nuclear modification factor of $\phi$ meson measured in 60-70% centrality class for Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.