cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.161563.v1/t11
title: "Figure 07b from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the W+jets VRs (a-f) and tt̄ VRs (g-i) after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or containing combinations having two W/Z bosons. Last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t4
title: "Figure 05d" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the (a–c) SRs, (d–f) W+jets CRs and (g–i) tt̄ CRs after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or that contain two W/Z bosons. The last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t5
title: "Figure 05e" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the (a–c) SRs, (d–f) W+jets CRs and (g–i) tt̄ CRs after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or that contain two W/Z bosons. The last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t7
title: "Figure 05g" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the (a–c) SRs, (d–f) W+jets CRs and (g–i) tt̄ CRs after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or that contain two W/Z bosons. The last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t8
title: "Figure 05h" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the (a–c) SRs, (d–f) W+jets CRs and (g–i) tt̄ CRs after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or that contain two W/Z bosons. The last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t9
title: "Figure 05i" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the (a–c) SRs, (d–f) W+jets CRs and (g–i) tt̄ CRs after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or that contain two W/Z bosons. The last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t12
title: "Figure 07c from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the W+jets VRs (a-f) and tt̄ VRs (g-i) after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or containing combinations having two W/Z bosons. Last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t13
title: "Figure 07d from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the W+jets VRs (a-f) and tt̄ VRs (g-i) after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or containing combinations having two W/Z bosons. Last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t14
title: "Figure 07e from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the W+jets VRs (a-f) and tt̄ VRs (g-i) after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or containing combinations having two W/Z bosons. Last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t15
title: "Figure 07f from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Distributions of the VLQ-candidate mass, m<sub>VLQ</sub>, in the W+jets VRs (a-f) and tt̄ VRs (g-i) after the fit to the background-only hypothesis. The columns correspond from left to right to the low-, middle-, and high-p<sub>T</sub><sup>W</sup> bins in each region.

Other includes remaining backgrounds from top quarks or containing combinations having two W/Z bosons. Last bin includes overflow.

Note: the 'Data' values in the table are normalized by the width of the bin to correspond to the number of events per 100 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t16
title: "Figure 06a" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Expected (background-only) and observed 95&percnt; CL upper limits on the VLQ coupling κ as functions of the VLQ mass m<sub>Q</sub>, for T-singlet (a) and Y-triplet (b) vector-like quarks. The green and yellow bands indicate the systematic uncertainties which are profiled in the fit for the observed upper limits. For the T-singlet model, the result of the latest ATLAS combination of searches for single vector-like top-quarks  is overlaid; this includes the decay modes T→H t and T→Z t. These interpretations are limited to parameter combinations for which the model corrections are valid, by restricting the VLQ relative width to Γ<sub>Q</sub>/m<sub>Q</sub> &lt; 0.5, as indicated by the grey dashed line.
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t17
title: "Figure 06b" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Expected (background-only) and observed 95&percnt; CL upper limits on the VLQ coupling κ as functions of the VLQ mass m<sub>Q</sub>, for T-singlet (a) and Y-triplet (b) vector-like quarks. The green and yellow bands indicate the systematic uncertainties which are profiled in the fit for the observed upper limits. For the T-singlet model, the result of the latest ATLAS combination of searches for single vector-like top-quarks  is overlaid; this includes the decay modes T→H t and T→Z t. These interpretations are limited to parameter combinations for which the model corrections are valid, by restricting the VLQ relative width to Γ<sub>Q</sub>/m<sub>Q</sub> &lt; 0.5, as indicated by the grey dashed line.
description: No data abstract available.
DOI: 10.17182/hepdata.161563.v1/t19
title: "Figure 10b from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Exclusion limit (at 95&percnt; CL) for (a) T-singlet and (b) Y-triplet, expressed in terms of an upper limit on the VLQ relative width Γ<sub>Q</sub>/m<sub>Q</sub>, within its validity range for the modelling used, as a function of the VLQ mass m<sub>Q</sub>. This is an alternative presentation of the upper limit set in terms of the coupling κ in Figure 6. As can be seen by the fact the interference-included and signal-only exclusion curves overlap almost entirely, the effect of neglecting the interference is negligible for the vector-like Y-quark.
description: No data abstract available.
DOI: 10.17182/hepdata.132638.v1/t1
title: "Figure 2" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The $v_2\{2k\}$ ($k = 1, ..., 5$) values as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t2
title: "Figure 3" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The relative differences $(v_2\{2k\}-v_2\{10\})/v_2\{10\}$ ($k = 1, ..., 4$) as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t3
title: "Figure 4" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The $h_1$ and the $h_2$ hydrodynamic probes as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t4
title: "Figure 5 (left)" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The ratios between the hydrodynamic probes and their Taylor expansions. The ratios are plotted as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t5
title: "Figure 5 (right)" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The ratios between the hydrodynamic probes and their Taylor expansions. The ratios are plotted as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t6
title: "Figure 6 (upper)" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The magnitudes of the measured skewness $\gamma_1^\textrm{exp}$ and "corrected" skewness $\gamma_{1,\textrm{corr}}^\textrm{exp}$ as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.132638.v1/t8
title: "Figure 6 (lower)" of "Higher-order moments of the elliptic flow distribution in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: The magnitudes of the measured superskewness $\gamma_3^\textrm{exp}$ and "corrected" superskewness $\gamma_{3,\textrm{corr}}^\textrm{exp}$ as functions of centrality in PbPb collisions at $\sqrt{s_{NN}}=5.02~\textrm{Te}\textrm{V}$. The measurement is performed with charged particles within the acceptance region.
description: The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, $v_{2}\{2k\}$, are measured up to the tenth order ($k = 5$) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of $\sqrt{s_{\rm{NN}}}=5.02~\textrm{Te}\textrm{V}$. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of $0.607~\textrm{nb}^{-1}$. A hierarchy is observed between the coefficients, with $v_{2}\{2\} &gt; v_{2}\{4\} \gtrsim v_{2}\{6\} \gtrsim v_{2}\{8\} \gtrsim v_{2}\{10\}$. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event $v_{2}$ distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.
DOI: 10.17182/hepdata.161563.v1/t18
title: "Figure 10a from Auxiliary material" of "Search for single production of vector-like quarks decaying into $W(\ellν)b$ in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Exclusion limit (at 95&percnt; CL) for (a) T-singlet and (b) Y-triplet, expressed in terms of an upper limit on the VLQ relative width Γ<sub>Q</sub>/m<sub>Q</sub>, within its validity range for the modelling used, as a function of the VLQ mass m<sub>Q</sub>. This is an alternative presentation of the upper limit set in terms of the coupling κ in Figure 6. As can be seen by the fact the interference-included and signal-only exclusion curves overlap almost entirely, the effect of neglecting the interference is negligible for the vector-like Y-quark.
description: No data abstract available.
DOI: 10.17182/hepdata.130959.v1/t1
title: "Figure 2, left UPSILON(2S)" of "Observation of the $\Upsilon$(3S) meson and suppression of $\Upsilon$ states in PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV"

description: Measured $R_\text{AA}$ for the $\Upsilon(2S)$ state as functions of PbPb collision centrality, integrated over the full kinematic range $p_\text{T}$ &lt; 30 GeV/c and |y| &lt; 2.4. The global uncertainty "PP MB" represents the pp luminosity and PbPb $N_\text{MB}$ combined uncertainties, whereas the global uncertainty "PP 2S" corresponds to the uncertainty on the $\Upsilon(2S)$ pp yields.
description: The production of $\Upsilon(2S)$ and $\Upsilon(3S)$ mesons in lead-lead ($\text{PbPb}$) and proton-proton ($\text{pp}$) collisions is studied in their dimuon decay channel using the CMS detector at the LHC. The $\Upsilon(3S)$ meson is observed for the first time in \PbPb collisions, with a significance above five standard deviations. The nuclear modification factors, derived from the ratio of yields measured in $\text{PbPb}$ to $\text{pp}$ collisions, are reported for both $\Upsilon(2S)$ and $\Upsilon(3S)$ mesons as functions of $\Upsilon$ meson transverse momentum and $\text{PbPb}$ collision centrality. The suppression is found to be stronger for $\Upsilon(3S)$ mesons compared to $\Upsilon(2S)$ mesons, extending the pattern of sequential suppression of quarkonium states in nuclear collisions previously seen for the $J/\psi$, $\psi(2S)$, $\Upsilon(1S)$ and $\Upsilon(2S)$ mesons. The results provide new constraints on theoretical descriptions of the dynamics of quarkonium states in heavy ion collisions.