cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77893.v2/t122
title: "Acceptance and Efficiency 23" of "Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions"

description: Performance of the SR-8j80-1b for the 2Step grid: fractional acceptance; fractional efficiency.
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
DOI: 10.17182/hepdata.77893.v2/t123
title: "Acceptance and Efficiency 24" of "Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions"

description: Performance of the SR-8j80-2b for the 2Step grid: fractional acceptance; fractional efficiency.
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
DOI: 10.17182/hepdata.77893.v2/t124
title: "Acceptance and Efficiency 25" of "Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions"

description: Performance of the SR-9j80-0b for the 2Step grid: fractional acceptance; fractional efficiency.
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
DOI: 10.17182/hepdata.77893.v2/t125
title: "Acceptance and Efficiency 26" of "Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions"

description: Performance of the SR-9j80-1b for the 2Step grid: fractional acceptance; fractional efficiency.
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
DOI: 10.17182/hepdata.77893.v2/t126
title: "Acceptance and Efficiency 27" of "Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions"

description: Performance of the SR-9j80-2b for the 2Step grid: fractional acceptance; fractional efficiency.
description: CERN-LHC. A search is presented for particles that decay producing a large jet multiplicity and invisible particles. The event selection applies a veto on the presence of isolated electrons or muons and additional requirements on the number of $b$-tagged jets and the scalar sum of masses of large-radius jets. Having explored the full ATLAS 2015--2016 dataset of LHC proton--proton collisions at $\sqrt{s}$=13 TeV, which corresponds to 36.1~fb$^{-1}$ of integrated luminosity, no evidence is found for physics beyond the Standard Model.The results are interpreted in the context of simplified models inspired by R-parity-conserving and R-parity-violating supersymmetry, where gluinos are pair-produced. More generic models within the phenomenological minimal supersymmetric Standard Model are also considered.
DOI: 10.15468/dl.jaek7u
title: Occurrence Download

description: A dataset containing 50910 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Aves",
 "Year is 2024",
 "HasCoordinate is true",
 "Geometry POLYGON((-3.2 52.4, -2.3 52.4, -2.3 53.0, -3.2 53.0, -3.2 52.4))"
 ]
}

 The dataset includes 50910 records from 8 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015362-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.60707/ym31-xe02
title: OREX-803208-102 DIF
DOI: 10.60707/0g8c-8g04
title: OREX-803208-102 DIF
DOI: 10.15468/dl.9fxqfe
title: Occurrence Download

description: A dataset containing 1021 species occurrences available in GBIF matching the query:
{
 "and" : [
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Mysis oculata"
 ]
}

 The dataset includes 1021 records from 42 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015408-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.zcnfvw
title: Occurrence Download

description: A dataset containing 9613 species occurrences available in GBIF matching the query:
{
 "and" : [
 "OccurrenceStatus is Present",
 "TaxonKey is Trema tomentosum"
 ]
}

 The dataset includes 9613 records from 106 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015409-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.77904.v1/t1
title: "Table 1" of "Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV"

description: Invariant cross section of electrons from beauty-hadron decays as a function of transverse momentum in minimum-bias p--Pb collisions in the rapidity interval $-1.06 &lt; y_{\rm cms} &lt; 0.14$. The systematic uncertainties do not include an additional p--Pb normalisation uncertainty of 3.7%.
description: CERN-LHC. The production of beauty hadrons was measured via semi-leptonic decays at mid-rapidity with the ALICE detector at the LHC in the transverse momentum interval $1
DOI: 10.17182/hepdata.77904.v1/t2
title: "Table 2" of "Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV"

description: Invariant yield of electrons from beauty-hadron decays as a function of transverse momentum in 20% most central Pb--Pb collisions.
description: CERN-LHC. The production of beauty hadrons was measured via semi-leptonic decays at mid-rapidity with the ALICE detector at the LHC in the transverse momentum interval $1
DOI: 10.17182/hepdata.77904.v1/t3
title: "Table 3" of "Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV"

description: Nuclear modification factor $R_{\text{pA}}$ of electrons from beauty-hadron decays as a function of transverse momentum for minimum-bias p--Pb collisions in the rapidity interval $-1.06 &lt; y_{\rm cms} &lt; 0.14$. The systematic uncertainties do not include a global normalisation uncertainty of 5.1%.
description: CERN-LHC. The production of beauty hadrons was measured via semi-leptonic decays at mid-rapidity with the ALICE detector at the LHC in the transverse momentum interval $1
DOI: 10.17182/hepdata.77904.v1/t4
title: "Table 4" of "Measurement of electrons from beauty-hadron decays in p-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV and Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=2.76}$ TeV"

description: Nuclear modification factor $R_{\text{AA}}$ of electrons from beauty-hadron decays as a function of transverse momentum for 20% most central Pb--Pb collisions in the rapidity interval $-0.8 &lt; y_{\rm cms} &lt; 0.8$. The systematic uncertainties do not include a global normalisation uncertainty of 5.25%.
description: CERN-LHC. The production of beauty hadrons was measured via semi-leptonic decays at mid-rapidity with the ALICE detector at the LHC in the transverse momentum interval $1
DOI: 10.17182/hepdata.77971.v1/t1
title: "Table 1" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Average charged particle pseudo-rapidity density, $\langle\rm{d}N_{\rm{ch}}/\rm{d}\eta_{\rm{lab}}\rangle$, measured at mid-rapidity in visible cross section event classes. Multiplicity classes are defined using the V0A estimator; values for $\langle\rm{d}N_{\rm{ch}}/\rm{d}\eta_{\rm{lab}}\rangle$ are corrected for vertexing and trigger efficiency. Since statistical uncertainties are negligible, only total systematic uncertainties are reported.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t2
title: "Table 2" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t3
title: "Table 3" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t4
title: "Table 4" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-60% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t5
title: "Table 5" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t6
title: "Table 6" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t7
title: "Table 7" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20\% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t8
title: "Table 8" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40\% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t9
title: "Table 9" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60\% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t10
title: "Table 10" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100\% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t11
title: "Table 11" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Sigma^{*\pm}+\overline{\Sigma}^{*\mp}$)/4 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t12
title: "Table 12" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Mean $p_{\rm T}$ of $\Sigma^{*\pm}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t13
title: "Table 13" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Xi^{*0}+\overline{\Xi}^{0})$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t14
title: "Table 14" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Mean $p_{\rm T}$ of $\Xi^{*0}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t15
title: "Table 15" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Integrated yield ratio.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t16
title: "Table 16" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Integrated yield ratio.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t17
title: "Table 17" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Integrated yield ratio.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v1/t18
title: "Table 18" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Integrated yield ratio.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v2/t1
title: "Table 1" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Average charged particle pseudo-rapidity density, $\langle\rm{d}N_{\rm{ch}}/\rm{d}\eta_{\rm{lab}}\rangle$, measured at mid-rapidity in visible cross section event classes. Multiplicity classes are defined using the V0A estimator; values for $\langle\rm{d}N_{\rm{ch}}/\rm{d}\eta_{\rm{lab}}\rangle$ are corrected for vertexing and trigger efficiency. Since statistical uncertainties are negligible, only total systematic uncertainties are reported.
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v2/t2
title: "Table 2" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v2/t3
title: "Table 3" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v2/t4
title: "Table 4" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-60% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.
DOI: 10.17182/hepdata.77971.v2/t5
title: "Table 5" of "Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: $p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100% multiplicity class).
description: CERN-LHC. Transverse momentum spectra of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ produced in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV, measured in the rapidity range -0.5 &lt; $y_{\rm{CMS}}$ &lt; 0 with the ALICE detector at the LHC.