cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.103857.v1/t37
title: "v1 as a function of eta for different centralities (11.5 GeV)" of "Bulk Properties of the System Formed in Au+Au Collisions at $\sqrt{s_{\mathrm{NN}}}$ = 14.5 GeV"

description: Rapidity-odd charged particles directed flow v1 as a function of pseudorapidity $\eta$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 GeV for 0–10%, 10–40% and 40–80% centrality intervals.
description: BNL-STAR. Data from the paper "Bulk Properties of the System Formed in Au+Au Collisions at $\sqrt{s_{NN}}$ = 14.5 GeV". Systematic measurements of bulk properties of the system created in Au+Au collisions at $\sqrt{s_{NN}}$ = 14.5 GeV recorded by the STAR detector at the Relativistic Heavy Ion Collider (RHIC). The transverse momentum spectra of $\pi^{\pm}$, $K^{\pm}$ and p (p-bar) are studied at mid-rapidity (|y| &lt; 0.1) for nine centrality intervals. The centrality, transverse momentum ($p_{T}$), and pseudorapidity ($\eta$) dependence of inclusive charged particle elliptic flow (v2), and rapidity-odd charged particles directed flow (v1) results near mid-rapidity are also presented. These measurements are compared with the published results from Au+Au collisions at other energies, and from Pb+Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV. The results at $\sqrt{s_{NN}}$ = 14.5 GeV show similar behavior as established at other energies and fit well in the energy dependence trend. These results are important as the 14.5 GeV energy fills the gap in $\mu_{B}$, which is of the order of 100 MeV, between $\sqrt{s_{NN}}$ =11.5 and 19.6 GeV. Comparisons of the data with UrQMD and AMPT models show poor agreement in general.
DOI: 10.17182/hepdata.103857.v1/t41
title: "v1 as a function of eta for different centralities (39.0 GeV)" of "Bulk Properties of the System Formed in Au+Au Collisions at $\sqrt{s_{\mathrm{NN}}}$ = 14.5 GeV"

description: Rapidity-odd charged particles directed flow v1 as a function of pseudorapidity $\eta$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 39.0 GeV for 0–10%, 10–40% and 40–80% centrality intervals.
description: BNL-STAR. Data from the paper "Bulk Properties of the System Formed in Au+Au Collisions at $\sqrt{s_{NN}}$ = 14.5 GeV". Systematic measurements of bulk properties of the system created in Au+Au collisions at $\sqrt{s_{NN}}$ = 14.5 GeV recorded by the STAR detector at the Relativistic Heavy Ion Collider (RHIC). The transverse momentum spectra of $\pi^{\pm}$, $K^{\pm}$ and p (p-bar) are studied at mid-rapidity (|y| &lt; 0.1) for nine centrality intervals. The centrality, transverse momentum ($p_{T}$), and pseudorapidity ($\eta$) dependence of inclusive charged particle elliptic flow (v2), and rapidity-odd charged particles directed flow (v1) results near mid-rapidity are also presented. These measurements are compared with the published results from Au+Au collisions at other energies, and from Pb+Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV. The results at $\sqrt{s_{NN}}$ = 14.5 GeV show similar behavior as established at other energies and fit well in the energy dependence trend. These results are important as the 14.5 GeV energy fills the gap in $\mu_{B}$, which is of the order of 100 MeV, between $\sqrt{s_{NN}}$ =11.5 and 19.6 GeV. Comparisons of the data with UrQMD and AMPT models show poor agreement in general.
DOI: 10.17182/hepdata.104408.v1/t1
title: "Figure 3-a (7 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t2
title: "Figure 3-a (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t4
title: "Figure 3-a (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t5
title: "Figure 3-b (7 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t6
title: "Figure 3-b (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t10
title: "Additional Figure 1 (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t11
title: "Additional Figure 1 (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t12
title: "Additional Figure 7a" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The cluster efficiency in bins of hadronic and EM energy in region A. Region A is defined as 391 cm $&lt; r &lt;$ 695.5 cm and 400 cm $&lt; |z| &lt;$ 671 cm. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bins correspond to LLPs that decayed leptonically with 0 hadronic energy. The cluster efficiency includes all cluster-level selections described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 35% and 20% for region A and B, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t13
title: "Additional Figure 7b" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The cluster efficiency in bins of hadronic and EM energy in region B. Region B is defined as 671 cm $&lt; |z| &lt;$ 1100 cm, $r &lt;$ 695.5 cm, and $|\eta| &lt;$ 2. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bins correspond to LLPs that decayed leptonically with 0 hadronic energy. The cluster efficiency includes all cluster-level selections described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 35% and 20% for region A and B, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t7
title: "Figure 3-b (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t8
title: "Figure 3-b (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t9
title: "Additional Figure 1 (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t14
title: "Additional Figure 8" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The efficiency of $N_{station} &gt; 1$ requirement in bins of hadronic energy in region B. Region B is defined as 671 cm $&lt; |z| &lt;$ 1100 cm, $r &lt;$ 695.5 cm, and $|\eta| &lt;$ 2. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bin corresponds to LLPs that decayed leptonically with 0 hadronic energy. The efficiency is calculated with respect to clusters that pass all cluster-level cuts described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 10%.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v1/t3
title: "Figure 3-a (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t2
title: "Figure 3-a (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t3
title: "Figure 3-a (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t4
title: "Figure 3-a (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t5
title: "Figure 3-b (7 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t6
title: "Figure 3-b (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t1
title: "Figure 3-a (7 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t10
title: "Additional Figure 1 (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t12
title: "Additional Figure 7a" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The cluster efficiency in bins of hadronic and EM energy in region A. Region A is defined as 391 cm $&lt; r &lt;$ 695.5 cm and 400 cm $&lt; |z| &lt;$ 671 cm. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bins correspond to LLPs that decayed leptonically with 0 hadronic energy. The cluster efficiency includes all cluster-level selections described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 35% and 20% for region A and B, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t13
title: "Additional Figure 7b" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The cluster efficiency in bins of hadronic and EM energy in region B. Region B is defined as 671 cm $&lt; |z| &lt;$ 1100 cm, $r &lt;$ 695.5 cm, and $|\eta| &lt;$ 2. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bins correspond to LLPs that decayed leptonically with 0 hadronic energy. The cluster efficiency includes all cluster-level selections described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 35% and 20% for region A and B, respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t8
title: "Figure 3-b (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t9
title: "Additional Figure 1 (15 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t11
title: "Additional Figure 1 (55 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t15
title: "Additional Figure 9" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The geometric signal acceptance as a function of $c\tau$. The acceptance is shown for four different LLP mass hypotheses: 7, 15, 40, and 55 GeV. The acceptance is defined by requiring at least 1 LLP to decay in the region defined as 400 cm $&lt; |z| &lt;$ 1100 cm, $r &lt; $ 695.5 cm, and $|\eta| &lt;$ 2.4.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t7
title: "Figure 3-b (40 GeV)" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.104408.v2/t14
title: "Additional Figure 8" of "Search for long-lived particles decaying in the CMS endcap muon detectors in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The efficiency of $N_{station} &gt; 1$ requirement in bins of hadronic energy in region B. Region B is defined as 671 cm $&lt; |z| &lt;$ 1100 cm, $r &lt;$ 695.5 cm, and $|\eta| &lt;$ 2. The cluster efficiency is estimated with LLPs decaying to $\tau^{+} \tau^{-}$. The sample contains equal fractions of events with LLP mass of 7, 15, 40, and 55 GeV and LLP lifetime of 0.1, 1, 10, and 100m. The first hadronic energy bin corresponds to LLPs that decayed leptonically with 0 hadronic energy. The efficiency is calculated with respect to clusters that pass all cluster-level cuts described in the paper, except for the jet veto, time cut, and $\Delta\phi$ cut. The full simulation signal yield prediction for samples with various LLP mass between 7 - 55 GeV, lifetime between 0.1 - 100 m, and decay mode to $d\bar{d}$ and $\tau^{+} \tau^{-}$ can be reproduced using this parameterization to within 10%.
description: No data abstract available.
DOI: 10.17182/hepdata.104458.v1/t1
title: "Table of contents" of "Search for charginos and neutralinos in final states with two boosted hadronically decaying bosons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: - - - - - - - - Overview of HEPData Record - - - - - - - - <br><br> <b>Cutflow:</b> table<br><br> <b>Boson tagging:</b> $W/Z\rightarrow qq$ tagging efficiency $W/Z\rightarrow qq$ tagging rejection $Z/h\rightarrow bb$ tagging efficiency $Z/h\rightarrow bb$ tagging rejection $W\rightarrow qq$ tagging efficiency (vs official WP) $W\rightarrow qq$ tagging rejection (vs official WP) $Z\rightarrow qq$ tagging efficiency (vs official WP) $Z\rightarrow qq$ tagging rejection (vs official WP) <b>Systematic uncertainty:</b> table<br><br> <b>Summary of SR yields:</b> table<br><br> <b>Expected background yields and the breakdown:</b> CR0L / SR CR1L / VR1L /CR1Y / VR1Y <b>SR distributions:</b> SR-4Q-VV: Effective mass SR-4Q-VV: Leading jet mass SR-4Q-VV: Leading jet $D_{2}$ SR-4Q-VV: Sub-leading jet mass SR-4Q-VV: Sub-leading jet $D_{2}$ SR-2B2Q-VZ: $m_{\textrm{T2}}$ SR-2B2Q-VZ: bb-tagged jet mass SR-2B2Q-VZ: Effective mass SR-2B2Q-Vh: $m_{\textrm{T2}}$ SR-2B2Q-Vh: bb-tagged jet mass SR-2B2Q-Vh: Effective mass <b>Exclusion limit:</b> $(\tilde{W},~\tilde{B})$-SIM model (C1C1-WW): Expected limit Expected limit ($+1\sigma_{\textrm{exp}}$) Expected limit ($-1\sigma_{\textrm{exp}}$): (No mass point could be excluded) Observed limit Observed limit ($+1\sigma_{\textrm{theory}}^{\textrm{SUSY}}$) Observed limit ($-1\sigma_{\textrm{theory}}^{\textrm{SUSY}}$) $(\tilde{W},~\tilde{B})$-SIM model (C1N2-WZ): Expected limit Expected limit ($+1\sigma_{\textrm{exp}}$) Expected limit ($-1\sigma_{\textrm{exp}}$) Observed limit Observed limit ($+1\sigma_{\textrm{theory}}^{\textrm{SUSY}}$)
description: No data abstract available.
DOI: 10.17182/hepdata.104458.v1/t2
title: "Cut flows for the representative signals" of "Search for charginos and neutralinos in final states with two boosted hadronically decaying bosons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Cut flows of some representative signals up to SR-4Q-VV, SR-2B2Q-VZ, and SR-2B2Q-Vh. One signal point from the $(\tilde{W},~\tilde{B})$ simplified models (C1C1-WW, C1N2-WZ, and C1N2-Wh) and $(\tilde{H},~\tilde{G})$ is chosen. The "preliminary event reduction" is a technical selection applied for reducing the sample size, which is fully efficient after the $n_{\textrm{Large}-R~\textrm{jets}}\geq 2$ selection.
description: No data abstract available.
DOI: 10.17182/hepdata.104458.v1/t3
title: "$W/Z\rightarrow qq$ tagging efficiency" of "Search for charginos and neutralinos in final states with two boosted hadronically decaying bosons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The boson-tagging efficiency for jets arising from $W/Z$ bosons decaying into $q\bar{q}$ (signal jets) are shown. The signal jet efficiency of $W_{qq}$/$Z_{qq}$-tagging is evaluated using a sample of pre-selected large-$R$ jets ($p_{\textrm{T}}&gt;200~\textrm{GeV}, |\eta|&lt;2.0, m_{J} &gt; 40~\textrm{GeV}$) in the simulated $(\tilde{W},\tilde{B})$ simplified model signal events with $\Delta m (\tilde{\chi}_{\textrm{heavy}},~\tilde{\chi}_{\textrm{light}}) \ge 400~\textrm{GeV}$. The jets are matched with generator-level $W/Z$-bosons by $\Delta R&lt;1.0$ which decay into $q\bar{q}$. The efficiency correction factors are applied on the signal efficiency rejection for the $W_{qq}$/$Z_{qq}$-tagging. The systematic uncertainty is represented by the hashed bands.
description: No data abstract available.
DOI: 10.17182/hepdata.104458.v1/t4
title: "$W/Z\rightarrow qq$ tagging rejection" of "Search for charginos and neutralinos in final states with two boosted hadronically decaying bosons and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: The rejection factor (inverse of the efficiency) for jets that have the other origins (background jets) are shown. The background jet rejection factor is calculated using pre-selected large-$R$ jets in the sample of simulated $Z\rightarrow\nu\nu$ + jets events, dominated by initial state radiation (ISR) jets. The efficiency correction factors are applied on the background rejection for the $W_{qq}$/$Z_{qq}$-tagging. The systematic uncertainty is represented by the hashed bands.
description: No data abstract available.