cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130966.v1/t2
title: "Inclusive signal strength correlation matrix" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of the signal strength modifiers corresponding to the four main SM H boson production mechanisms.
description: No data abstract available.
DOI: 10.17182/hepdata.130966.v1/t3
title: "Likelihood scan for overall signal strength" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Profile likelihood as a function of the overall HWW signal strength modifier, considering all uncertainties
description: No data abstract available.
DOI: 10.17182/hepdata.130966.v1/t4
title: "Likelihood scan (stat. unc.) for overall signal strength" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Profile likelihood as a function of the overall HWW signal strength modifier, considering statistical uncertainties only
description: No data abstract available.
DOI: 10.17182/hepdata.130966.v1/t5
title: "2D likelihood scan for kappas" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: 2D likelihood profile as a function of kappa_v and kappa_f
description: No data abstract available.
DOI: 10.17182/hepdata.130966.v1/t6
title: "STXS signal strenght modifiers and cross sections" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The measured product of cross section times branching fraction for HWW decay and the SM predictions for the merged Stage 1.2 STXS production bins at mH = 125.38 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.130966.v1/t7
title: "STXS signal strength correlation matrix" of "Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of the signal strength modifiers corresponding to the Stage 1.2 STXS production bins at mH = 125.38 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.130967.v1/t1
title: "Hypertriton production yield" of "Hypertriton production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Integrated yield of hypertriton produced in 0-40% p-Pb collisions
description: The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of $^{3}_{\Lambda}\text{H}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval $-1 &lt; y &lt; 0$ for the 40% highest multiplicity p-Pb collisions is $\mathrm{d} N /\mathrm{d} y =[\mathrm{6.3 \pm 1.8 (stat.) \pm 1.0 (syst.) ] \times 10^{-7}}$.The measurement is compared with the expectations of statistical hadronisation and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in small collision systems such as p-Pb and therefore the measurement of $\mathrm{d} N /\mathrm{d} y$ is crucial to distinguish between them.The precision of this measurement leads to the exclusion with a significance larger than 6$\sigma$ of some configurations of the statistical hadronisation, thus constraining the production mechanism of loosely bound states.
DOI: 10.17182/hepdata.130967.v1/t2
title: "Hypertriton over $\Lambda$ ratio" of "Hypertriton production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Hypertriton over $\Lambda$ ratio in 0-40% p-Pb collisions
description: The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of $^{3}_{\Lambda}\text{H}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval $-1 &lt; y &lt; 0$ for the 40% highest multiplicity p-Pb collisions is $\mathrm{d} N /\mathrm{d} y =[\mathrm{6.3 \pm 1.8 (stat.) \pm 1.0 (syst.) ] \times 10^{-7}}$.The measurement is compared with the expectations of statistical hadronisation and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in small collision systems such as p-Pb and therefore the measurement of $\mathrm{d} N /\mathrm{d} y$ is crucial to distinguish between them.The precision of this measurement leads to the exclusion with a significance larger than 6$\sigma$ of some configurations of the statistical hadronisation, thus constraining the production mechanism of loosely bound states.
DOI: 10.17182/hepdata.130967.v1/t3
title: "$S_3$" of "Hypertriton production in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $S_3$ in the 40% largest multiplicity p-Pb collisions
description: The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of $^{3}_{\Lambda}\text{H}$ in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval $-1 &lt; y &lt; 0$ for the 40% highest multiplicity p-Pb collisions is $\mathrm{d} N /\mathrm{d} y =[\mathrm{6.3 \pm 1.8 (stat.) \pm 1.0 (syst.) ] \times 10^{-7}}$.The measurement is compared with the expectations of statistical hadronisation and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in small collision systems such as p-Pb and therefore the measurement of $\mathrm{d} N /\mathrm{d} y$ is crucial to distinguish between them.The precision of this measurement leads to the exclusion with a significance larger than 6$\sigma$ of some configurations of the statistical hadronisation, thus constraining the production mechanism of loosely bound states.
DOI: 10.17182/hepdata.131043.v2/t1
title: "Figure 3a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: M_ttH which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t2
title: "Figure 3b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta \eta_{B-B}, which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t3
title: "Figure 3c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta R_{jet-jet}, which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t4
title: "Figure 4a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: M_ttH which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc1sto1769453
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.131043.v2/t10
title: "Figure 7a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected likelihood scan as a function of kappa_t and #tilde{kappa_t}
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t5
title: "Figure 4b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta \eta_{B-B}, which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t6
title: "Figure 4c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta R_{l1-l2}, which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t7
title: "Figure 6a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 2lss + 0 au category
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t8
title: "Figure 6b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 3l +0 au category
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t11
title: "Figure 7b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed likelihood scan as a function of kappa_t and #tilde{kappa_t}
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t12
title: "Figure 8" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Likelihood scan as a function of |f_{CP}^{Htt}| for multilepton final states
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t13
title: "Figure 9a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected likelihood scan as a function of |f_{CP}^{Htt}| for multilepton, #gamma#gamma+ZZ final states and the combniation.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t14
title: "Figure 9b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed likelihood scan as a function of |f_{CP}^{Htt}| for multilepton final states and the combniation.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t15
title: "Figure 10" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Likelihood scan as a function of kappa_t and #tilde{kappa_t} for multilepton final states and the combination with #gamma#gamma and ZZ final states.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v2/t9
title: "Figure 6c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 2lss + 1 au category
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t1
title: "Figure 3a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: M_ttH which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t2
title: "Figure 3b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta \eta_{B-B}, which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t3
title: "Figure 3c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta R_{jet-jet}, which is one of the input variables to the XGBoost used for CP discrimination in 2lss + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t4
title: "Figure 4a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: M_ttH which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t5
title: "Figure 4b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta \eta_{B-B}, which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t6
title: "Figure 4c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: \Delta R_{l1-l2}, which is one of the input variables to the XGBoost used for CP discrimination in 3l + 0tau channel, defined in table 4.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t7
title: "Figure 6a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 2lss + 0 au category
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc1sto1769845
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.131043.v1/t10
title: "Figure 7a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected likelihood scan as a function of kappa_t and #tilde{kappa_t}
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t11
title: "Figure 7b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed likelihood scan as a function of kappa_t and #tilde{kappa_t}
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t12
title: "Figure 8" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Likelihood scan as a function of |f_{CP}^{Htt}| for multilepton final states
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t13
title: "Figure 9a" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Expected likelihood scan as a function of |f_{CP}^{Htt}| for multilepton, #gamma#gamma+ZZ final states and the combniation.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t8
title: "Figure 6b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 3l +0 au category
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t9
title: "Figure 6c" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Postfit discriminating distributions used as input to the fit. Events in the tH{} node are caregorized in bins of CP discriminant in the 2lss + 1 au category
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t14
title: "Figure 9b" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed likelihood scan as a function of |f_{CP}^{Htt}| for multilepton final states and the combniation.
description: No data abstract available.
DOI: 10.17182/hepdata.131043.v1/t15
title: "Figure 10" of "Search for $CP$ violation in ttH and tH production in multilepton channels in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Likelihood scan as a function of kappa_t and #tilde{kappa_t} for multilepton final states and the combination with #gamma#gamma and ZZ final states.
description: No data abstract available.
DOI: 10.17182/hepdata.131222.v1/t1
title: "Table 1" of "Measurement of exclusive pion pair production in proton-proton collisions at $\sqrt{s}=$7 TeV with the ATLAS detector"

description: The measured fiducial cross sections. The first systematic uncertainty is the combined systematic uncertainty excluding luminosity, the second is the luminosity
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t1
title: "Table 1" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t2
title: "Table 2" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t3
title: "Table 3" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t4
title: "Table 4" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t5
title: "Table 5" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t6
title: "Table 6" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t7
title: "Table 7" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t8
title: "Table 8" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.25549/vercoutere-ouc1sto1769461
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.131260.v1/t10
title: "Table 10" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t11
title: "Table 11" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t12
title: "Table 12" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t9
title: "Table 9" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t13
title: "Table 13" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.
DOI: 10.17182/hepdata.131260.v1/t14
title: "Table 14" of "Neutral to charged kaon yield fluctuations in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV"

description: No table description available.
description: No data abstract available.