cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.114367.v1/t10
title: "Observed 95% CL upper limits for Wprime signal" of "Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on $\sigma \mathcal{B}$(W' -&gt; ZW) as a function of the resonance mass, taking into account all statistical and systematic uncertainties. The electron and muon channels and the various categories used in the analysis are combined. The inner green band and the outer yellow band represent the 68 and 95% coverage of the expected limits in the background-only hypothesis.
description: A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.
DOI: 10.17182/hepdata.114367.v1/t11
title: "Observed 95% CL upper limits on ALP linear couplings" of "Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the product of the ALP coupling to gluons and the coupling to Z bosons as a function of the mass scale $f_a$ for ALP masses smaller than 100 GeV.
description: A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.
DOI: 10.17182/hepdata.114367.v1/t12
title: "Observed 95% CL upper limits on ALP chiral couplings" of "Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on the product of the ALP coupling to gluons and the chiral $a_\widetilde{2D}$ coupling as a function of the mass scale $f_a$ for ALP masses smaller than 100 GeV.
description: A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.
DOI: 10.17182/hepdata.114367.v1/t9
title: "Observed 95% CL upper limits for bulk graviton signal" of "Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limit on $\sigma \mathcal{B}$(G -&gt; ZZ) as a function of the resonance mass, taking into account all statistical and systematic uncertainties. The electron and muon channels and the various categories used in the analysis are combined. The inner green band and the outer yellow band represent the 68 and 95% coverage of the expected limits in the background-only hypothesis.
description: A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.
DOI: 10.17182/hepdata.114370.v4/t2
title: "Figure 4. Transverse momentum distribution for B meson" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: Transverse momentum distribution for B-candidate
description: No data abstract available.
DOI: 10.17182/hepdata.114367.v1/t8
title: "SR2 diboson mass resolved tagged category" of "Search for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production at $\sqrt{s}$ = 13 TeV"

description: SR2 diboson invariant mass distribution in the resolved tagged category after fitting the signal and sideband regions using a signal (ALP chiral ZH) plus background model. The last bin includes events with diboson invariant masses up to 3000 GeV. The signal is normalized to the 95% CL cross section limit at $f_a$ = 3 TeV (the scale factor used in the original figure for better visibility is not applied here).
description: A search has been performed for heavy resonances decaying to ZZ or ZW and axion-like particles mediating nonresonant ZZ or ZH production in semileptonic final states, with two charged leptons (electrons or muons) produced by the decay of a Z boson, and two quarks produced by the decay of a Z, W, or Higgs boson H. The analysis is sensitive to resonances with masses in the range from 450 to 1800 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying boson. The search is based on data collected during 2016 to 2018 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 137 $\text{fb}^{-1}$. No significant excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as functions of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet and warped extra dimensions model, respectively. In addition, upper limits on the ALP-mediated diboson production cross section and ALP couplings to standard model particles are obtained in the framework of linear and chiral effective field theories.
DOI: 10.17182/hepdata.114370.v1/t1
title: "Table 1. Results for the ratios of braching fractions" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: The measured branching fraction ratios
description: No data abstract available.
DOI: 10.17182/hepdata.114370.v1/t2
title: "Figure 4. Transverse momentum distribution for B meson" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: Transverse momentum distribution for B-candidate
description: No data abstract available.
DOI: 10.17182/hepdata.114370.v2/t1
title: "Table 1. Results for the ratios of braching fractions" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: The measured branching fraction ratios
description: No data abstract available.
DOI: 10.17182/hepdata.114370.v2/t2
title: "Figure 4. Transverse momentum distribution for B meson" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: Transverse momentum distribution for B-candidate
description: No data abstract available.
DOI: 10.17182/hepdata.114370.v3/t1
title: "Table 1. Results for the ratios of braching fractions" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: The measured branching fraction ratios
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc110610347
title: Therapeutic Artworks

description: This collection includes over 900 pieces of art that were created by patients at the Atascadero State Hospital (ASH) in the mid-1950’s.  The artists were under the treatment of Albert R. Vercoutere who used the technique of providing photos from magazines for the patients to use as inspiration for their own artwork. Although not trained in the use of art therapy and during a time when art therapy was a new approach, Vercoutere often utilized art as a mechanism for working with his patients. The artwork was created during a time when psychotropic drugs were not yet available as treatment options for mental health patients.
DOI: 10.17182/hepdata.114370.v3/t2
title: "Figure 4. Transverse momentum distribution for B meson" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: Transverse momentum distribution for B-candidate
description: No data abstract available.
DOI: 10.17182/hepdata.114370.v3/t3
title: "Table 2. Results for the ratios of braching fractions" of "Observation of B$^0$$\to$$\psi$(2S)K$^0_\mathrm{S}\pi^+\pi^-$ and B$^0_\mathrm{S}$$\to$$\psi$(2S)K$^0_\mathrm{S}$ decays"

description: The measured branching fractions
description: No data abstract available.
DOI: 10.17182/hepdata.114371.v1/t1
title: "Figure 3" of "Measurement of cold nuclear matter effects for inclusive $J/\psi$ in $p$+Au collisions at $\sqrt{s_{_{\mathrm{NN}}}}$ = 200 GeV"

description: Inclusive J/psi cross section times branching ratio of the dimuon decay channel in p+p collisions at 200 GeV. Global uncertainty of 12.5% not shown.
description: Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive \jpsi\ at mid-rapidity in 0-100\% \pAu\ collisions at \sqrtsNN\ = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, \rpa, obtained by taking a ratio of \jpsi\ yield in \pAu\ collisions to that in \pp\ collisions scaled by the number of binary nucleon-nucleon collisions. The differential \jpsi\ yield in both \pp\ and \pAu\ collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the \jpsi\ \rpa\ is derived within the transverse momentum (\pT) range of 0 to 10 \gev. A suppression of approximately 30\% is observed for $\pT&lt;2$ \gev, while \jpsi\ \rpa\ becomes compatible with unity for \pT\ greater than 3 \gev, indicating the \jpsi\ yield is minimally affected by the CNM effects at high \pT. Comparison to a similar measurement from 0-20\% central \AuAu\ collisions reveals that the observed strong \jpsi\ suppression above 3 \gev\ is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured \jpsi\ \rpa, while their agreement with the \jpsi\ yields in \pp\ and \pAu\ collisions is worse.
DOI: 10.17182/hepdata.114371.v1/t2
title: "Figure 4" of "Measurement of cold nuclear matter effects for inclusive $J/\psi$ in $p$+Au collisions at $\sqrt{s_{_{\mathrm{NN}}}}$ = 200 GeV"

description: Inclusive J/psi cross section times branching ratio of the dimuon decay channel in p+Au collisions at 200 GeV. Global uncertainty of 1.5% not shown.
description: Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive \jpsi\ at mid-rapidity in 0-100\% \pAu\ collisions at \sqrtsNN\ = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, \rpa, obtained by taking a ratio of \jpsi\ yield in \pAu\ collisions to that in \pp\ collisions scaled by the number of binary nucleon-nucleon collisions. The differential \jpsi\ yield in both \pp\ and \pAu\ collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the \jpsi\ \rpa\ is derived within the transverse momentum (\pT) range of 0 to 10 \gev. A suppression of approximately 30\% is observed for $\pT&lt;2$ \gev, while \jpsi\ \rpa\ becomes compatible with unity for \pT\ greater than 3 \gev, indicating the \jpsi\ yield is minimally affected by the CNM effects at high \pT. Comparison to a similar measurement from 0-20\% central \AuAu\ collisions reveals that the observed strong \jpsi\ suppression above 3 \gev\ is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured \jpsi\ \rpa, while their agreement with the \jpsi\ yields in \pp\ and \pAu\ collisions is worse.
DOI: 10.17182/hepdata.114371.v1/t3
title: "Figure 5" of "Measurement of cold nuclear matter effects for inclusive $J/\psi$ in $p$+Au collisions at $\sqrt{s_{_{\mathrm{NN}}}}$ = 200 GeV"

description: R_pAu of inclusive J/psi in p+Au collisions at 200 GeV. Global uncertainty of 13.9% not shown.
description: Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive \jpsi\ at mid-rapidity in 0-100\% \pAu\ collisions at \sqrtsNN\ = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, \rpa, obtained by taking a ratio of \jpsi\ yield in \pAu\ collisions to that in \pp\ collisions scaled by the number of binary nucleon-nucleon collisions. The differential \jpsi\ yield in both \pp\ and \pAu\ collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the \jpsi\ \rpa\ is derived within the transverse momentum (\pT) range of 0 to 10 \gev. A suppression of approximately 30\% is observed for $\pT&lt;2$ \gev, while \jpsi\ \rpa\ becomes compatible with unity for \pT\ greater than 3 \gev, indicating the \jpsi\ yield is minimally affected by the CNM effects at high \pT. Comparison to a similar measurement from 0-20\% central \AuAu\ collisions reveals that the observed strong \jpsi\ suppression above 3 \gev\ is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured \jpsi\ \rpa, while their agreement with the \jpsi\ yields in \pp\ and \pAu\ collisions is worse.
DOI: 10.17182/hepdata.114372.v1/t1
title: "Table 1" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: The measured $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes from STAR (2021)
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t3
title: "Table 3" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy of $^{4}_{\Lambda}$H vs y in 3 GeV 0-10% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.25549/vercoutere-ouc110610363
title: 3 women and 2 men plus word salad

description: Three orange nude females standing (one with blond hair with one arm raised; one with brown hair with arms down; and one with blond hair with both arms up); two orange nude males with brown hair depicted from the waist up standing in the foreground; area around the figures is dark green, blue, and tan; remainder of the page is unpainted; word salad printed in red covers the remainder of the page including some words printed between the figures, one section printed perpendicular to the other words. See description of 347 for OT notes.
DOI: 10.17182/hepdata.114372.v1/t2
title: "Table 2" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy of $^{3}_{\Lambda}$H vs y in 3 GeV 0-10% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t4
title: "Table 4" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy of $^{3}_{\Lambda}$H vs y in 3 GeV 10-50% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t5
title: "Table 5" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy of $^{4}_{\Lambda}$H vs y in 3 GeV 10-50% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t6
title: "Table 6" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy at |y|&lt;0.5 of $^{3}_{\Lambda}$H vs B.R in 3 GeV 0-10% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t7
title: "Table 7" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: B.R. times dN/dy at |y|&lt;0.5 of $^{4}_{\Lambda}$H vs B.R in 3 GeV 0-10% Au+Au collisions
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t12
title: "Table 12" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: $^{4}_{\Lambda}$H $p_T$ spectra times B.R., -0.25
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.
DOI: 10.17182/hepdata.114372.v1/t13
title: "Table 13" of "Measurements of ${}^3_\Lambda \rm{H}$ and ${}^4_\Lambda \rm{H}$ Lifetimes and Yields in Au+Au Collisions in the High Baryon Density Region"

description: $^{4}_{\Lambda}$H $p_T$ spectra times B.R., -0.5
description: STAR-RHIC. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H lifetimes are measured with $\sqrt{s_{\rm NN}}=3.0$ GeV and $\sqrt{s_{\rm NN}}=7.2$ GeV data taken using the fixed-target mode. $^{3}_{\Lambda}$H and $^{4}_{\Lambda}$H $dN/dy$ and $p_{T}$ spectra at $\sqrt{s_{\rm NN}}=3.0$ GeV are also presented.