cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.131308.v1/t23
title: "Figure_008-a" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=0.01mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.17182/hepdata.131308.v1/t24
title: "Figure_008-b" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=0.05mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.17182/hepdata.131308.v1/t25
title: "Figure_008-c" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=0.1mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.17182/hepdata.131308.v1/t26
title: "Figure_008-d" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=0.5mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.25549/vercoutere-ouc110610622
title: 2 nude men and 1 nude woman and a table

description: Two nude males and one nude female sitting on a wood table in a room with green walls, brown framed windows, and a wooden floor. See description of 001 for OT notes.
DOI: 10.17182/hepdata.131308.v1/t27
title: "Figure_008-e" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=1mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.17182/hepdata.131308.v1/t28
title: "Figure_008-f" of "Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed 95% CL cross section upper limits as a function of the stau mass for long-lived staus in the maximally-mixed stau scenario for m(LSP)=1 GeV and ctau_0(stau)=2.5mm
description: A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $\tau$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $\tau$ sleptons decay promptly, the search also addresses scenarios in which the $\tau$ sleptons have sufficiently long lifetimes to give rise to nonprompt $\tau$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016--2018, and correspond to an integrated luminosity of 138\fbinv. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $\tau$ sleptons are obtained in the framework of simplified models. In a scenario in which the $\tau$ sleptons are superpartners of left-handed $\tau$ leptons, and each undergoes a prompt decay to a $\tau$ lepton and a nearly massless LSP, $\tau$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $\tau$ sleptons corresponds to $c\tau=0.1$ mm, where $\tau_{0}$ represents the mean proper lifetime of the $\tau$ slepton, masses between 150 and 220 GeV are excluded.
DOI: 10.15468/dl.v9jyw3
title: Occurrence Download

description: A dataset listing the 932 species recorded in GBIF matching the query:
{
 "and" : [
 "Country is Mexico",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Marchantiophyta"
 ]
}

 The dataset's 932 records were derived from 69 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015954-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.131521.v1/t1
title: "Table 1" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Average signal on A-side vs. C-side ZN in pp collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t2
title: "Table 2" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Average signal on A-side vs. C-side ZP in pp collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t3
title: "Table 3" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Pb-remnant side ZN signal normalized to MB value vs. ZN centrality percentile in p-Pb collisions at 5.02 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t4
title: "Table 4" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Pb-remnant side ZN signal normalized to MB value vs. ZN centrality percentile in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t5
title: "Table 5" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: p-remnant side ZN signal normalized to MB value vs. ZN centrality percentile in p-Pb collisions at 5.02 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t6
title: "Table 6" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: p-remnant side ZN signal normalized to MB value vs. ZN centrality percentile in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t7
title: "Table 7" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Pb-remnant side ZN signal normalized to MB value vs. average Ncoll in p-Pb collisions at 5.02 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t8
title: "Table 8" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: Pb-remnant side ZN signal normalized to MB value vs. average Ncoll in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t10
title: "Table 10" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: p-remnant side ZN signal normalized to MB value vs. average Ncoll in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t11
title: "Table 11" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: ZN signal normalized to MB value vs. normalized charged-particle multiplicity in p-p collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t12
title: "Table 12" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: p-remnant side ZN signal normalized to MB value vs. normalized charged-particle multiplicity in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t13
title: "Table 13" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: ZP signal normalized to MB value vs. normalized charged-particle multiplicity in p-p collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t14
title: "Table 14" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: p-remnant side ZP signal normalized to MB value vs. average charged-particle multiplicity in p-Pb collisions at 8.16 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t15
title: "Table 15" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: ZN signal normalized to MB value vs. leading transverse momentum in |eta|&lt;0.8 in p-p collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.
DOI: 10.17182/hepdata.131521.v1/t16
title: "Table 16" of "Measurement of very forward energy and particle production at midrapidity in pp and p-Pb collisions at the LHC"

description: ZP signal normalized to MB value vs. leading transverse momentum in |eta|&lt;0.8 in p-p collisions at 13 TeV
description: Event characterization in pp and p-Pb collisions thorough the measurement of the very forward energy detected by the ZDC. Energy detected in the neutron (ZN) and proton (ZP) zero-degree calorimeters are correlated to activity measured at midrapidity and in particular with: - multiplicity of charged particles produced in |eta|&lt;1 - transverse momentum of particle with highest pt, pt leading, in |eta|&lt;0.8.