cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.155678.v1/t154
title: "Cutflow 6" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM2 using the $m(\tilde{t}_{1},\tilde{\chi}_{1}^{0}) = (750,450)$ GeV signal point as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t155
title: "Cutflow 7" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM3 using the $m(\tilde{t}_{1},\tilde{\chi}_{1}^{0}) = (750,450)$ GeV signal point as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t156
title: "Cutflow 8" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM-Disc using the $m(\tilde{t}_{1},\tilde{\chi}_{1}^{0}) = (750,450)$ GeV signal point as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t157
title: "Cutflow 9" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM1 using the $m(\mathrm{LQ}_{21}^\mathrm{u}) = 600$ GeV signal point, with a 50% branching fraction to $c\nu$, as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t158
title: "Cutflow 10" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM2 using the $m(\mathrm{LQ}_{21}^\mathrm{u}) = 600$ GeV signal point, with a 50% branching fraction to $c\nu$, as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t159
title: "Cutflow 11" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM3 using the $m(\mathrm{LQ}_{21}^\mathrm{u}) = 600$ GeV signal point, with a 50% branching fraction to $c\nu$, as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155678.v1/t160
title: "Cutflow 12" of "Search for supersymmetry in final states with missing transverse momentum and charm-tagged jets using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Cutflow table for SR-HM-Disc using the $m(\mathrm{LQ}_{21}^\mathrm{u}) = 600$ GeV signal point, with a 50% branching fraction to $c\nu$, as the benchmark. All jet-related variables use jets with $p_\mathrm{T}&gt;40$ GeV, however, the $E_\mathrm{T}^\mathrm{miss}$ is calculated with jets with $p_\mathrm{T}&gt;20$ GeV. The "Preselection" requirement includes: $E_\mathrm{T}^\mathrm{miss}&gt;250$ GeV; events containing electrons or muons are vetoed; at least two jets must be present of which at least one must be identified as a $c$-tagged jet; events with jets that have been identified as $b$-tagged are discarded; the minimum azimuthal angular ($\phi$) distance between the (up to) four leading jets and the $\vec{p}_\mathrm{T}^\mathrm{miss}$ is required to be greater than 0.4.
description: The paper presents a search for supersymmetric particles produced in proton-proton collisions at $\sqrt{s}=13$ TeV and decaying into final states with missing transverse momentum and jets originating from charm quarks. The data were taken with the ATLAS detector at the Large Hadron Collider at CERN from 2015 to 2018 and correspond to an integrated luminosity of 139 fb$^{-1}$. No significant excess of events over the expected Standard Model background expectation is observed in optimized signal regions, and limits are set on the production cross-sections of the supersymmetric particles. Pair production of charm squarks or top squarks, each decaying into a charm quark and the lightest supersymmetric particle $\tilde{\chi}_1^0$, is excluded at 95% confidence level for squarks with masses up to 900 GeV for scenarios where the mass of $\tilde{\chi}_1^0$ is below 50 GeV. Additionally, the production of leptoquarks with masses up to 900 GeV is excluded for the scenario where up-type leptoquarks decay into a charm quark and a neutrino. Model-independent limits on cross-sections and event yields for processes beyond the Standard Model are also reported.
DOI: 10.17182/hepdata.155679.v1/t1
title: "Net-Xi-net-K Correlation pp" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in pp collisions at $\sqrt{s} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t2
title: "Net-Xi-net-K Correlation p-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t3
title: "Net-Xi-net-K Correlation Pb-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t4
title: "Net-Xi cumulant ratio pp" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in pp collisions at $\sqrt{s} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t10
title: "Covariance matrix net-Xi net-K correlation Pb-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t5
title: "Net-Xi cumulant ratio p-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t6
title: "Net-Xi cumulant ratio Pb-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t7
title: "Chi square profile" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: $\chi^2$ profile obtained from the simultaneous comparison of the ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$ and $\rho_{\Delta\Xi\Delta\mathrm{K}}$ measured in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV with model calculations carried out with the Thermal-FIST code, for different values of the volume parameter $V_{\mathrm{c}}$
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t8
title: "Covariance matrix net-Xi net-K correlation pp" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in pp collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t9
title: "Covariance matrix net-Xi net-K correlation p-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the Pearson correlation coefficient between the net-$\Xi$ number and net-K number, $\rho_{\Delta\Xi\Delta\mathrm{K}}$, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t11
title: "Covariance matrix net-Xi cumulant ratio pp" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in pp collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t12
title: "Covariance matrix net-Xi cumulant ratio p-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155679.v1/t13
title: "Covariance matrix net-Xi cumulant ratio Pb-Pb" of "Probing strangeness hadronization with event-by-event production of multistrange hadrons"

description: Covariance matrix of the normalized second-order cumulant of the Net-$\Xi$ number, ${\kappa}_{2}(\overline{\Xi}^{+} - \Xi^{-})/{\kappa}_{1}(\overline{\Xi}^{+} + \Xi^{-})$, in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV
description: No data abstract available.
DOI: 10.17182/hepdata.155693.v1/t1
title: "Figure 2a" of "Measurement of the inclusive WZ production cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV"

description: Number of events for the different lepton flavour categories in the ZZ control region accounting for the fit to data. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other" category
description: No data abstract available.
DOI: 10.17182/hepdata.155693.v1/t2
title: "Figure 4a" of "Measurement of the inclusive WZ production cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV"

description: Number of events for the different lepton flavour categories in the ttZ control region accounting for the fit to data. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other" category
description: No data abstract available.
DOI: 10.17182/hepdata.155693.v1/t3
title: "Figure 5a" of "Measurement of the inclusive WZ production cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV"

description: Number of events for the different lepton flavour categories in the X+#gamma control region accounting for the fit to data. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other" category
description: No data abstract available.
DOI: 10.17182/hepdata.155693.v1/t4
title: "Figure 6a" of "Measurement of the inclusive WZ production cross section in pp collisions at $\sqrt{s}$ = 13.6 TeV"

description: Number of events for the different lepton flavour categories in the signal region accounting for the fit to data. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other" category
description: No data abstract available.