cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.145071.v2/t2
title: "Table 2" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of non-prompt $J/\psi$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t3
title: "Table 3" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of prompt $\psi(2S)$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t4
title: "Table 4" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for cross-section of non-prompt $\psi(2S)$ decaying to a muon pair for 13 TeV data in fb/GeV. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t5
title: "Table 5" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt fraction of $J/\psi$ decaying to a muon pair as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t6
title: "Table 6" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt fraction of $\psi(2S)$ decaying to a muon pair as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t7
title: "Table 7" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for prompt $\psi(2S)$ over $J/\psi$ ratio as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t8
title: "Table 8" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of results for non-prompt $\psi(2S)$ over $J/\psi$ ratio as a percentage for 13 TeV data. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145071.v2/t9
title: "Table 9" of "Measurement of the production cross-section of $J/\psi$ and $\psi(2$S$)$ mesons in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Correction factors for an assumed angular dependence $\propto 1+\lambda_{\theta} \cos^2\theta $ in the helicity frame, for several values of the parameter $\lambda_{\theta}$. The correction factors were found to be the same (within 1% - 2%) for $J/\psi$ and $\psi(2S)$ mesons, for prompt and non-prompt production mechanisms, and for the three rapidity intervals considered in this paper.
description: CERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 140 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=13$ TeV. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity.
DOI: 10.17182/hepdata.145072.v1/t1
title: "Table 0: Acceptance times Efficiency, lephad" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: Acceptance $\times$ efficiency for the $\tau_\text{lep}\tau_\text{had}$ signal region assuming $\beta$ = 0.5 as a function of m$_\text{LQ}$.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t2
title: "Table 1: Acceptance times Efficiency, hadhad" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: Acceptance $\times$ efficiency for the $\tau_\text{had}\tau_\text{had}$ signal region assuming $\beta$ = 0.5 as a function of m$_\text{LQ}$.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t3
title: "Table 2: Scalar LQ Cross-Section Limits" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: The observed and expected 95% CL upper limits on the scalar LQ pair production cross-sections assuming B = 1 as a function of m$_\text{LQ}$.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t4
title: "Table 3: Minimal Vector LQ Cross-Section Limits" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: The observed and expected 95% CL upper limits on the minimal coupling vector LQ pair production cross-sections assuming B = 1 as a function of m$_\text{LQ}$.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t5
title: "Table 4: Yang-Mills Vector LQ Cross-Section Limits" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: The observed and expected 95% CL upper limits on the Yang-Mills coupling vector LQ pair production cross-sections assuming B = 1 as a function of m$_\text{LQ}$.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t6
title: "Table 5: Limits on B(LQ-&gt;b+tau) v.s. Scalar LQ Mass" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: The observed and expected 95% CL upper limits on the branching ratio into charged leptons as a function of m$_\text{LQ}$ for the scalar LQ.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.
DOI: 10.17182/hepdata.145072.v1/t7
title: "Table 6: Limits on B(LQ-&gt;b+tau) v.s. Minimal Vector LQ Mass" of "Search for pair production of third-generation leptoquarks decaying into a bottom quark and a $\tau$-lepton with the ATLAS detector"

description: The observed and expected 95% CL upper limits on the branching ratio into charged leptons as a function of m$_\text{LQ}$ for the vector LQ minimal coupling scenario.
description: CERN-LHC, ATLAS. A search for pair-produced scalar or vector leptoquarks (LQs) decaying into a $b$-quark and a $\tau$-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb$^{\text{-1}}$ collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV. Events in which at least one $\tau$-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of m$_\text{LQ}$ and branching ratio B into a $\tau$-lepton and $b$-quark. For scalar LQs, masses below 1460 GeV are excluded assuming B = 100%, while for vector LQs the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang-Mills, YM) scenario.

Basic event selection:
- ==0(1) electron or muon for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ thresholds are corresponding trigger, in fiducial volume, isolated from jets
- ==1(2) hadronically decaying $\tau$s ($\tau_{had}$s) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region: $p_T$ &gt; 100 GeV (thresholds are corresponding trigger) for $\tau_\text{lep}\tau_\text{had}$ ($\tau_\text{had}\tau_\text{had}$) region, in fiducial volume, isolated from jets
- &gt;=2 small-R jets, with 1 or 2 $b$-tagged
- Opposite charge electron/muon/$\tau_{had}$s and $\tau_{had}$s
- MMC mass from 2 leptons ($m_{MMC}$) should be not 40 &lt; $m_{MMC}$ &lt; 150 GeV (Z veto)
- Missing transverse momentum &gt; 100 GeV
- Scalar sum of $p_T$ ($s_T$) &gt; 600 GeV

See paper for more detail.