cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.96305.v1/t5
title: "Figure 25a" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_2/K_1$ plotted as a function of the mean number of participants $$ for two rapidity acceptances
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t6
title: "Figure 25b" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_3/K_2$ plotted as a function of the mean number of participants $$ for two rapidity acceptances
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t7
title: "Figure 25c" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_4/K_2$ plotted as a function of the mean number of participants $$ for two rapidity acceptances
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t8
title: "Figure 26a" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant $K_2$ plotted as a function of $\Delta y$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t9
title: "Figure 26b" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant $K_3$ plotted as a function of $\Delta y$
description: No data abstract available.
DOI: 10.3535/8y3-1dx-s02
title: Fagus sylvatica L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/fj6-j2z-3c7
title: Logfia minima (Sm.) Dumort.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96305.v1/t10
title: "Figure 26c" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant $K_4$ plotted as a function of $\Delta y$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t11
title: "Figure 26e" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_3$ plotted as a function of $\Delta y$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t12
title: "Figure 26f" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_4$ plotted as a function of $\Delta y$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t13
title: "Figure 27 top" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_2$ plotted as a function of maximum $p_t$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t14
title: "Figure 27 middle" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_3$ plotted as a function of maximum $p_t$
description: No data abstract available.
DOI: 10.3535/f77-5ex-4qw
title: Juncus effusus L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/zt5-dhk-2ry
title: Calluna vulgaris (L.) Hull

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96305.v1/t15
title: "Figure 27 bottom" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_4$ plotted as a function of maximum $p_t$
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t16
title: "Figure 28a" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_2$ plotted as a function of the mean number of protons.
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t17
title: "Figure 28b" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_3$ plotted as a function of the mean number of protons.
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t18
title: "Figure 28c" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton correlator $C_4$ plotted as a function of the mean number of protons.
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t19
title: "Figure 29 left" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_3/K_2$ plotted as a function of the center-of-mass energy for two centrality bins (0-10% and 30-40%).
description: No data abstract available.
DOI: 10.17182/hepdata.96305.v1/t20
title: "Figure 29 right" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_4/K_2$ plotted as a function of the center-of-mass energy for two centrality bins (0-10% and 30-40%).
description: No data abstract available.
DOI: 10.3535/31g-ny6-8yp
title: Acer campestre L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/5h1-g75-kg3
title: Teesdalia nudicaulis (L.) W. T. Aiton

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/p2j-acj-asl
title: Rumex acetosella L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96305.v1/t3
title: "Figure 22middle" of "Proton number fluctuations in $\sqrt{s_{NN}}$ = 2.4 GeV Au+Au collisions studied with HADES"

description: Efficiency and N2LO volume-corrected proton cumulant ratio $K_3/K_2$ plotted as a function of the rapidity acceptance
description: No data abstract available.
DOI: 10.17182/hepdata.96389.v1/t1
title: "Table 1: LQLQ-&gt;tete Cross Section Limit" of "Search for pair production of scalar leptoquarks decaying into first- or second-generation leptons and top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed upper limits at the 95% CL on the leptoquark pair production cross section as a function of leptoquark mass under the assumption of $\mathcal{B}$(LQ-&gt;$te$)=1.
description: Limits on pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark. The search is based on 139.0 $\pm$ 2.4 fb$^{-1}$ of pp collisions at $\sqrt{s}$ = 13 TeV recorded in 2015-2018 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the fully hadronic top quark final state, with a focus on the high LQ mass regime for which the top quarks tend to be boosted. The search results are interpreted to provide a limit on the leptoquark mass. Mass limits on leptoquark pair production are also set as a function of the leptoquark decay branching ratio into a charged lepton and a top quark, as opposed to a neutrino and a bottom quark. 

Basic event selection:
- == 2 opposite-sign same-flavour leptons: pT &gt; 100 GeV, in fiducial volume, isolated from jets 
- &gt;= 2 large-radius jets
- dilepton invariant mass &gt; 120 GeV

A parameterized boosted decision tree classifier is used to optimize the sensitivity to LQ signal, using event kinematics and jet substructure variables (see paper).
DOI: 10.17182/hepdata.96389.v1/t2
title: "Table 2: LQLQ-&gt;tmutmu Cross Section Limit" of "Search for pair production of scalar leptoquarks decaying into first- or second-generation leptons and top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed upper limits at the 95% CL on the leptoquark pair production cross section as a function of leptoquark mass under the assumption of $\mathcal{B}$(LQ-&gt;$t\mu$)=1.
description: Limits on pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark. The search is based on 139.0 $\pm$ 2.4 fb$^{-1}$ of pp collisions at $\sqrt{s}$ = 13 TeV recorded in 2015-2018 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the fully hadronic top quark final state, with a focus on the high LQ mass regime for which the top quarks tend to be boosted. The search results are interpreted to provide a limit on the leptoquark mass. Mass limits on leptoquark pair production are also set as a function of the leptoquark decay branching ratio into a charged lepton and a top quark, as opposed to a neutrino and a bottom quark. 

Basic event selection:
- == 2 opposite-sign same-flavour leptons: pT &gt; 100 GeV, in fiducial volume, isolated from jets 
- &gt;= 2 large-radius jets
- dilepton invariant mass &gt; 120 GeV

A parameterized boosted decision tree classifier is used to optimize the sensitivity to LQ signal, using event kinematics and jet substructure variables (see paper).
DOI: 10.17182/hepdata.96389.v1/t3
title: "Table 3: Limit on LQ mass vs. B(LQ-&gt;te)" of "Search for pair production of scalar leptoquarks decaying into first- or second-generation leptons and top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed 95% CL lower limits on the leptoquark mass as a function of the branching ratio $\mathcal{B}$(LQ-&gt;$te$).
description: Limits on pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark. The search is based on 139.0 $\pm$ 2.4 fb$^{-1}$ of pp collisions at $\sqrt{s}$ = 13 TeV recorded in 2015-2018 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the fully hadronic top quark final state, with a focus on the high LQ mass regime for which the top quarks tend to be boosted. The search results are interpreted to provide a limit on the leptoquark mass. Mass limits on leptoquark pair production are also set as a function of the leptoquark decay branching ratio into a charged lepton and a top quark, as opposed to a neutrino and a bottom quark. 

Basic event selection:
- == 2 opposite-sign same-flavour leptons: pT &gt; 100 GeV, in fiducial volume, isolated from jets 
- &gt;= 2 large-radius jets
- dilepton invariant mass &gt; 120 GeV

A parameterized boosted decision tree classifier is used to optimize the sensitivity to LQ signal, using event kinematics and jet substructure variables (see paper).
DOI: 10.17182/hepdata.96389.v1/t4
title: "Table 4: Limit on LQ mass vs. B(LQ-&gt;tmu)" of "Search for pair production of scalar leptoquarks decaying into first- or second-generation leptons and top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed 95% CL lower limits on the leptoquark mass as a function of the branching ratio $\mathcal{B}$(LQ-&gt;$t\mu$).
description: Limits on pair production of scalar leptoquarks, each decaying into either an electron or a muon and a top quark. The search is based on 139.0 $\pm$ 2.4 fb$^{-1}$ of pp collisions at $\sqrt{s}$ = 13 TeV recorded in 2015-2018 with the ATLAS detector at the CERN Large Hadron Collider. Data are analysed in the fully hadronic top quark final state, with a focus on the high LQ mass regime for which the top quarks tend to be boosted. The search results are interpreted to provide a limit on the leptoquark mass. Mass limits on leptoquark pair production are also set as a function of the leptoquark decay branching ratio into a charged lepton and a top quark, as opposed to a neutrino and a bottom quark. 

Basic event selection:
- == 2 opposite-sign same-flavour leptons: pT &gt; 100 GeV, in fiducial volume, isolated from jets 
- &gt;= 2 large-radius jets
- dilepton invariant mass &gt; 120 GeV

A parameterized boosted decision tree classifier is used to optimize the sensitivity to LQ signal, using event kinematics and jet substructure variables (see paper).
DOI: 10.17182/hepdata.96390.v1/t1
title: "Combined NN output distribution in CRZ$\tau\tau$, $\mu\tau$ 1P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the CRZ$\tau\tau$ for the $\mu\tau$ channel for events with 1-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.3535/b24-mnh-vrh
title: Capsella bursa-pastoris (L.) Medik.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.3535/erx-tps-qby
title: Anchusa officinalis L.

description: Digital Specimen for the physical specimen hosted at Botanic Garden and Botanical Museum Berlin.
DOI: 10.17182/hepdata.96390.v1/t2
title: "Combined NN output distribution in CRZ$\tau\tau$, $\mu\tau$ 3P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the CRZ$\tau\tau$ for the $\mu\tau$ channel for events with 3-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.17182/hepdata.96390.v1/t3
title: "Combined NN output distribution in VRSS, $e\tau$ 1P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the VRSS for the $e\tau$ channel for events with 1-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.17182/hepdata.96390.v1/t4
title: "Combined NN output distribution in VRSS, $e\tau$ 3P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the VRSS for the $e\tau$ channel for events with 3-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.17182/hepdata.96390.v1/t5
title: "Combined NN output distribution in SR, $e\tau$ 1P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the SR for the $e\tau$ channel for events with 1-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.17182/hepdata.96390.v1/t6
title: "Combined NN output distribution in SR, $e\tau$ 3P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the SR for the $e\tau$ channel for events with 3-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}
DOI: 10.17182/hepdata.96390.v1/t7
title: "Combined NN output distribution in SR, $\mu\tau$ 1P" of "Search for charged-lepton-flavour violation in $Z$-boson decays with the ATLAS detector"

description: The best-fit expected and observed distributions of the combined NN output in the SR for the $\mu\tau$ channel for events with 1-prong $\tau_\text{had-vis}$ candidates. The last bin in each plot includes overflow events.
description: A search for $Z$ boson decays into a $\tau$ lepton and another lepton of different flavour ($\ell$) with opposite electric charge is presented.
The data analysed correspond to $139\text{ fb}^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=13\text{ TeV}$ and $20.3\text{ fb}^{-1}$ at $\sqrt{s}=8\text{ TeV}$, recorded with the ATLAS detector at the LHC.

Events are categorised according to the multiplicities and kinematics of reconstructed electrons, muons and $\tau$ leptons, as well as the missing transverse momentum.

The signal region (SR) is defined by a $e^\pm\tau^\mp$ or $\mu^\pm\tau^\mp$ final state with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&lt;35\text{ GeV}$.

The same-sign validation region (VRSS) is defined similarly to the SR but with a $e^\pm\tau^\pm$ or $\mu^\pm\tau^\pm$ final state.

The control region enhanced in $Z\rightarrow\tau\tau$ events (CRZ$\tau\tau$) is defined similarly to the SR but with $m_\mathrm{T}(\tau_\mathrm{had-vis}, E_\mathrm{T}^\mathrm{miss})&gt;35\text{ GeV}$, $m_\mathrm{T}(\ell, E_\mathrm{T}^\mathrm{miss})&lt;40$ GeV and $70\text{ GeV}