cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105510.v1/t108
title: "Table 108 from Fig 12" of "Beam energy dependence of (anti-)deuteron production in Au+Au collisions at RHIC"

description: 'Coalescence parameter $B_{2}$ as a function of $m_{T}$ $-$ $m_{0}$ for deuterons (left panel)'
description: We report the energy dependence of mid-rapidity (anti-)deuteron production in Au+Au collisions at $\sqrt{s_\text{NN}} =\ $7.7, 11.5, 14.5, 19.6, 27, 39, 62.4, and 200 GeV, measured by the STAR experiment at RHIC. The yield of deuterons is found to be well described by the thermal model. The collision energy, centrality, and transverse momentum dependence of the coalescence parameter $B_2$ are discussed. We find that the values of $B_2$ for anti-deuterons are systematically lower than those for deuterons, indicating that the correlation volume of anti-baryons is larger than that of baryons at $\sqrt{s_\text{NN}}$ from 19.6 to 39 GeV. In addition, values of $B_2$ are found to vary with collision energy and show a broad minimum around $\sqrt{s_\text{NN}}=\ $20 to 40 GeV, which might imply a change of the equation of state of the medium in these collisions.
DOI: 10.17182/hepdata.105510.v1/t109
title: "Table 109 from Fig 12" of "Beam energy dependence of (anti-)deuteron production in Au+Au collisions at RHIC"

description: 'Coalescence parameter $B_{2}$ as a function of $m_{T}$ $-$ $m_{0}$ for anti-deuterons (right panel)'
description: We report the energy dependence of mid-rapidity (anti-)deuteron production in Au+Au collisions at $\sqrt{s_\text{NN}} =\ $7.7, 11.5, 14.5, 19.6, 27, 39, 62.4, and 200 GeV, measured by the STAR experiment at RHIC. The yield of deuterons is found to be well described by the thermal model. The collision energy, centrality, and transverse momentum dependence of the coalescence parameter $B_2$ are discussed. We find that the values of $B_2$ for anti-deuterons are systematically lower than those for deuterons, indicating that the correlation volume of anti-baryons is larger than that of baryons at $\sqrt{s_\text{NN}}$ from 19.6 to 39 GeV. In addition, values of $B_2$ are found to vary with collision energy and show a broad minimum around $\sqrt{s_\text{NN}}=\ $20 to 40 GeV, which might imply a change of the equation of state of the medium in these collisions.
DOI: 10.17182/hepdata.105510.v1/t110
title: "Table 110 from Fig 13" of "Beam energy dependence of (anti-)deuteron production in Au+Au collisions at RHIC"

description: 'Energy dependence of the coalescence parameter for $B_{2}(d)$'
description: We report the energy dependence of mid-rapidity (anti-)deuteron production in Au+Au collisions at $\sqrt{s_\text{NN}} =\ $7.7, 11.5, 14.5, 19.6, 27, 39, 62.4, and 200 GeV, measured by the STAR experiment at RHIC. The yield of deuterons is found to be well described by the thermal model. The collision energy, centrality, and transverse momentum dependence of the coalescence parameter $B_2$ are discussed. We find that the values of $B_2$ for anti-deuterons are systematically lower than those for deuterons, indicating that the correlation volume of anti-baryons is larger than that of baryons at $\sqrt{s_\text{NN}}$ from 19.6 to 39 GeV. In addition, values of $B_2$ are found to vary with collision energy and show a broad minimum around $\sqrt{s_\text{NN}}=\ $20 to 40 GeV, which might imply a change of the equation of state of the medium in these collisions.
DOI: 10.17182/hepdata.105510.v1/t111
title: "Table 111 from Fig 13" of "Beam energy dependence of (anti-)deuteron production in Au+Au collisions at RHIC"

description: 'Energy dependence of the coalescence parameter for $B_{2}(\bar{d})$'
description: We report the energy dependence of mid-rapidity (anti-)deuteron production in Au+Au collisions at $\sqrt{s_\text{NN}} =\ $7.7, 11.5, 14.5, 19.6, 27, 39, 62.4, and 200 GeV, measured by the STAR experiment at RHIC. The yield of deuterons is found to be well described by the thermal model. The collision energy, centrality, and transverse momentum dependence of the coalescence parameter $B_2$ are discussed. We find that the values of $B_2$ for anti-deuterons are systematically lower than those for deuterons, indicating that the correlation volume of anti-baryons is larger than that of baryons at $\sqrt{s_\text{NN}}$ from 19.6 to 39 GeV. In addition, values of $B_2$ are found to vary with collision energy and show a broad minimum around $\sqrt{s_\text{NN}}=\ $20 to 40 GeV, which might imply a change of the equation of state of the medium in these collisions.
DOI: 10.17182/hepdata.105516.v1/t1
title: "Combined NN output in SR, $e\tau_\mu$ low-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the combined NN output in the low-$p_\text{T}$-SR for the $e\tau_\mu$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t2
title: "Combined NN output in SR, $\mu\tau_e$ low-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the combined NN output in the low-$p_\text{T}$-SR for the $\mu\tau_e$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t3
title: "Combined NN output in SR, $e\tau_\mu$ high-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the combined NN output in the high-$p_\text{T}$-SR for the $e\tau_\mu$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t10
title: "Collinear mass in CRZ$\tau\tau$, $\mu\tau_e$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the collinear mass $m_\text{coll}$ in the CRZ$\tau\tau$ for the $\mu\tau_e$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t4
title: "Combined NN output in SR, $\mu\tau_e$ high-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the combined NN output in the high-$p_\text{T}$-SR for the $\mu\tau_e$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t5
title: "Collinear mass in SR, $e\tau_\mu$ high-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the collinear mass $m_\text{coll}$ in the high-$p_\text{T}$-SR for the $e\tau_\mu$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t6
title: "Collinear mass in SR, $\mu\tau_e$ high-$p_\text{T}$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the collinear mass $m_\text{coll}$ in the high-$p_\text{T}$-SR for the $\mu\tau_e$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t7
title: "Upper limits on $\mathcal{B}(Z\to\ell\tau)$, $\tau\to\ell\nu\nu$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: Observed and expected upper limits on $\mathcal{B}(Z\rightarrow\ell\tau)$ with leptonically decaying $\tau$ at 95% confidence level.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t8
title: "Upper limits on $\mathcal{B}(Z\rightarrow\ell\tau)$, combined" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: Observed and expected upper limits on $\mathcal{B}(Z\rightarrow\ell\tau)$ at 95% confidence level, combination of hadronically and leptonically decaying $\tau$ channels.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.17182/hepdata.105516.v1/t9
title: "Collinear mass in CRZ$\tau\tau$, $e\tau_\mu$" of "Search for lepton-flavor-violation in $Z$-boson decays with $\tau$-leptons with the ATLAS detector"

description: The best-fit predicted and observed distributions of the collinear mass $m_\text{coll}$ in the CRZ$\tau\tau$ for the $e\tau_\mu$ channel. The first and last bin include underflow and overflow events, respectively.
description: CERN-LHC. Search for lepton-flavor-violating $Z\to e\tau$ and $Z\to\mu\tau$ decays with 139 fb$^{-1}$ of Run 2 $pp$ collision data at a center-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. This search exploits leptonically-decaying taus in the final state and is combined with a similar ATLAS search in the final state in which the tau-lepton decays hadronically using the same data set as well as Run 1 data. Final states with an opposite-sign electron-muon pair are considered.

The fiducial region of the $e\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 10 GeV
- $p_{\mathrm{T}}(e)$ &gt; $p_{\mathrm{T}}(\mu)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(e,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(\mu,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV

The fiducial region of the $\mu\tau$ channel is defined as:
- Opposite-sign electron-muon pair
- $p_{\mathrm{T}}(e)$ &gt; 15 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; 27 GeV
- $p_{\mathrm{T}}(\mu)$ &gt; $p_{\mathrm{T}}(e)$
- Veto on 1.37 &lt; $|\eta(e)|$ &lt; 1.52
- $\Delta R(e,\mu)$ &gt; 0.1
- $|\Delta\phi(\mu,E^{\mathrm{miss}}_{\mathrm{T}})|$ &gt; 1
- Visible mass $m_{\mathrm{vis}}(e,\mu)$ &gt; 40 GeV
- No $b$-jets
- Transverse mass $m_{\mathrm{T}}(e,E^{\mathrm{miss}}_{\mathrm{T}})$ &lt; 35 GeV
DOI: 10.25549/vercoutere-ouc110610940
title: Very small human head

description: One very small human head in white with gray outline surrounded by a green and black with touches of blue background . See description of 001 for OT notes.