cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.144178.v2/t58
title: "Cutflow T5btbt (m(~g)=1.5 TeVm(~chi10)=1.1 TeVc#tau=10 cm)" of "Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Cut flow for model T1btbt (m(~g)=1.5 TeV, m(~chi10)=1.1 TeV, c#tau=10 cm), showing events passing each cut stage.
description: A search is presented for charged, long-lived supersymmetric particles in final states with one or more disappearing tracks. The search is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the CERN LHC between 2016 and 2018, corresponding to an integrated luminosity of 137/fb. The search is performed over final states characterized by varying numbers of jets, b-tagged jets, electrons, and muons. The length of signal-candidate tracks in the plane perpendicular to the beam axis is used to characterize the lifetimes of wino- and higgsino-like charginos produced in the context of the minimal supersymmetric standard model. The dE/dx energy loss of signal-candidate tracks is used to increase the sensitivity to charginos with a large mass and thus a small Lorentz boost. The observed results are found to be statistically consistent with the background-only hypothesis. Limits on the pair production cross section of gluinos and squarks are presented in the framework of simplified models of supersymmetric particle production and decay, and for electroweakino production based on models of wino and higgsino dark matter. The limits presented are the most stringent to date for scenarios with light third-generation squarks and a wino- or higgsino-like dark matter candidate capable of explaining the observed dark matter relic density.
DOI: 10.17182/hepdata.144178.v2/t59
title: "SR cutflow T6tb (m(~b)=1 TeVm(~chi10)=900 GeVc#tau=10 cm)" of "Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Cut flow for model T2tb (m(~b)=1 TeV, m(~chi10)=900 GeV, c#tau=10 cm), showing events passing each cut stage.
description: A search is presented for charged, long-lived supersymmetric particles in final states with one or more disappearing tracks. The search is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the CERN LHC between 2016 and 2018, corresponding to an integrated luminosity of 137/fb. The search is performed over final states characterized by varying numbers of jets, b-tagged jets, electrons, and muons. The length of signal-candidate tracks in the plane perpendicular to the beam axis is used to characterize the lifetimes of wino- and higgsino-like charginos produced in the context of the minimal supersymmetric standard model. The dE/dx energy loss of signal-candidate tracks is used to increase the sensitivity to charginos with a large mass and thus a small Lorentz boost. The observed results are found to be statistically consistent with the background-only hypothesis. Limits on the pair production cross section of gluinos and squarks are presented in the framework of simplified models of supersymmetric particle production and decay, and for electroweakino production based on models of wino and higgsino dark matter. The limits presented are the most stringent to date for scenarios with light third-generation squarks and a wino- or higgsino-like dark matter candidate capable of explaining the observed dark matter relic density.
DOI: 10.17182/hepdata.144178.v2/t60
title: "SR cutflow T5btbt (m(~g)=1.5 TeVm(~chi10)=1.1 TeVc#tau=10 cm)" of "Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Cut flow for model T1btbt (m(~g)=1.5 TeV, m(~chi10)=1.1 TeV, c#tau=10 cm), showing events passing each cut stage.
description: A search is presented for charged, long-lived supersymmetric particles in final states with one or more disappearing tracks. The search is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the CERN LHC between 2016 and 2018, corresponding to an integrated luminosity of 137/fb. The search is performed over final states characterized by varying numbers of jets, b-tagged jets, electrons, and muons. The length of signal-candidate tracks in the plane perpendicular to the beam axis is used to characterize the lifetimes of wino- and higgsino-like charginos produced in the context of the minimal supersymmetric standard model. The dE/dx energy loss of signal-candidate tracks is used to increase the sensitivity to charginos with a large mass and thus a small Lorentz boost. The observed results are found to be statistically consistent with the background-only hypothesis. Limits on the pair production cross section of gluinos and squarks are presented in the framework of simplified models of supersymmetric particle production and decay, and for electroweakino production based on models of wino and higgsino dark matter. The limits presented are the most stringent to date for scenarios with light third-generation squarks and a wino- or higgsino-like dark matter candidate capable of explaining the observed dark matter relic density.
DOI: 10.17182/hepdata.144179.v1/t1
title: "Figure 4a" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $R0_A$ control subregion for muons. The lower panel reports the data minus the expected number of events normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t2
title: "Figure 4b" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $R0_A$ control subregion for electrons. The lower panel reports the data minus the expected number of events normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t3
title: "Figure 5a" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $R2B_A$ subregion for muons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t4
title: "Figure 5b" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $R2B_A$ subregion for electrons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t5
title: "Figure 5c" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $RW'_A$ subregion for muons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t6
title: "Figure 5d" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $RW'_A$ subregion for electrons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t7
title: "Figure 5e" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $RT_A$ subregion for muons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t8
title: "Figure 5f" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Post-fit distributions of $M_{\ell v jj}$ in the $RT_A$ subregion for electrons. All process yields and nuisance parameters are set to the values obtained from the background plus signal fit. The signal considered for the fit corresponds to the purely right-handed production of a W' with $m_{W'}$ of 3.6 TeV and a relative width of 1$\%$ of the $m_{W'}$, and is represented by the solid red line. The lower panels show the data minus the expected number of events, normalized to the statistical uncertainty of the data. The orange band represents the systematic uncertainties, also normalized to the statistical uncertainty of the data.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.
DOI: 10.17182/hepdata.144179.v1/t10
title: "Figure 6b" of "Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed and expected 95% CL upper limits on the product of the production cross section for a left-handed production of a tb quark pair in the $s$-channel, mediated by a W or W' bosons and including interference terms, given as functions of $m_{W'}$ for a relative width of 10%. The inner (green) band and the outer (yellow) band indicate the regions containing 68 and 95%, respectively, of the distribution of limits expected under the background-only hypothesis. The solid red curves show the theoretical expectation at LO.
description: A search for W' bosons decaying to a top and a bottom quark in final states including electrons or muons is performed with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of $138~\mathrm{fb}^{-1}$ of proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. In general, good agreement with the standard model expectation is observed and no evidence for the existence of the W' boson is found over the mass range examined. The largest observed excess is found for a W' boson mass ($m_{\mathrm{W'}}$) hypothesis of $3.8~\mathrm{TeV}$ with a relative decay width of $1\%$, with a local (global) significance of $2.6$ $(2.0)$ standard deviations. Upper limits on the production cross sections of W' bosons decaying to a top and a bottom quark are set. Left- and right-handed W' bosons with $m_{\mathrm{W'}}$ below $3.9$ and $4.3~\mathrm{TeV}$, respectively, are excluded at the $95\%$ confidence level, under the assumption that the new particle has a narrow decay width. Limits are also set for relative decay widths up to $30\%$. These are the most stringent limits to date on W' bosons decaying to a top and a bottom quark.