cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.105516.v1/t11
title: "Combined NN output 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 combined NN output 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: 10.17182/hepdata.105516.v1/t12
title: "Combined NN output 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 combined NN output 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/t13
title: "Electron transverse momentum (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 leading lepton transverse momentum $p_\text{T}(e)$ 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/t14
title: "Muon transverse momentum 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 leading lepton transverse momentum $p_\text{T}(\mu)$ 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/t15
title: "Missing transverse momentum 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 missing transverse momentum $E^\text{miss}_\text{T}$ 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/t16
title: "Missing transverse momentum 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 missing transverse momentum $E^\text{miss}_\text{T}$ 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.105628.v1/t1
title: "Table 1 from Fig 3a" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer of $\Lambda$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t2
title: "Table 2 from Fig 3b" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer of $\bar{\Lambda}$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t3
title: "Table 3 from Fig 3c" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'spin asymmetry $\delta_{TT}$ for the control sample of $K_S^0$ meson.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t4
title: "Table 4 from Fig 4a" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer of $\Lambda$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t5
title: "Table 5 from Fig 4a" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer of $\bar{\Lambda}$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t6
title: "Table 6 from Fig 4b" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer $\Lambda$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.17182/hepdata.105628.v1/t7
title: "Table 7 from Fig 4b" of "Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$"

description: 'Transverse spin transfer of $\bar{\Lambda}$ in transversely polarized proton-proton collisions at 200 GeV.'
description: The transverse spin transfer from polarized protons to $\Lambda$ and $\bar{\Lambda}$ hyperons is expected to provide sensitivity to the transversity distribution of the nucleon and to the transversely polarized fragmentation functions. We report the first measurement of the transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ along the polarization direction of the fragmenting quark, $D_\mathrm{TT}$, in transversely polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$ with the STAR detector at RHIC. The data correspond to an integrated luminosity of $18\,\mathrm{pb}^{-1}$ and cover the pseudorapidity range $|\eta| &lt; 1.2$ and transverse momenta $p_{\mathrm{T}}$ up to $8\,\mathrm{GeV}/c$. The dependence on $p_\mathrm{T}$ and $\eta$ are presented. The $D_\mathrm{TT}$ results are found to be comparable with a model prediction, and are also consistent with zero within uncertainties.
DOI: 10.25549/vercoutere-ouc110609785
title: Grass-skirted women II

description: Backview of three females inbrown grass skirts with arms raised standing on a beach in front of waves rolling in from the ocean, palm tree, and gray structure. OT notes on reverse of painting "Patient likes this. Considers it the best he's ever done here." See description of 001 for OT notes.
DOI: 10.17182/hepdata.105629.v1/t1
title: "Table 1 from Fig 6" of "Measurements of the transverse-momentum-dependent cross sections of $J/\psi$ production at mid-rapidity in proton+proton collisions at $\sqrt{s} =$ 510 and 500 GeV with the STAR detector"

description: 'fiducial cross sections multiplied by the branching ratio as a function of $J/\Psi$ $p_T$'
description: We present measurements of the differential cross sections of inclusive $J/ψ$ meson production as a function of transverse momentum ($p_{T}^{J/ψ}$) using the $μ^{+}μ^{-}$ and $e^{+}e^{-}$ decay channels in proton+proton collisions at center-of-mass energies of 510 and 500 GeV, respectively, recorded by the STAR detector at the Relativistic Heavy Ion Collider. The measurement from the $μ^{+}μ^{-}$ channel is for 0 $&lt; p_{T}^{J/ψ} &lt;$ 9 GeV/$c$ and rapidity range $|y^{J/ψ}| &lt; $ 0.4, and that from the $e^{+}e^{-}$ channel is for 4 $&lt; p_{T}^{J/ψ} &lt;$ 20 GeV/$c$ and $|y^{J/ψ}| &lt; $ 1.0. The $ψ(2S)$ to $J/ψ$ ratio is also measured for 4 $&lt; p_{T}^{\rm meson} &lt;$ 12 GeV/$c$ through the $e^{+}e^{-}$ decay channel. Model calculations, which incorporate different approaches toward the $J/ψ$ production mechanism, are compared with experimental results and show reasonable agreement within uncertainties.
DOI: 10.17182/hepdata.105629.v1/t2
title: "Table 2 from Fig 6" of "Measurements of the transverse-momentum-dependent cross sections of $J/\psi$ production at mid-rapidity in proton+proton collisions at $\sqrt{s} =$ 510 and 500 GeV with the STAR detector"

description: 'full cross sections multiplied by the branching ratio as a function of $J/\Psi$ $p_T$ '
description: We present measurements of the differential cross sections of inclusive $J/ψ$ meson production as a function of transverse momentum ($p_{T}^{J/ψ}$) using the $μ^{+}μ^{-}$ and $e^{+}e^{-}$ decay channels in proton+proton collisions at center-of-mass energies of 510 and 500 GeV, respectively, recorded by the STAR detector at the Relativistic Heavy Ion Collider. The measurement from the $μ^{+}μ^{-}$ channel is for 0 $&lt; p_{T}^{J/ψ} &lt;$ 9 GeV/$c$ and rapidity range $|y^{J/ψ}| &lt; $ 0.4, and that from the $e^{+}e^{-}$ channel is for 4 $&lt; p_{T}^{J/ψ} &lt;$ 20 GeV/$c$ and $|y^{J/ψ}| &lt; $ 1.0. The $ψ(2S)$ to $J/ψ$ ratio is also measured for 4 $&lt; p_{T}^{\rm meson} &lt;$ 12 GeV/$c$ through the $e^{+}e^{-}$ decay channel. Model calculations, which incorporate different approaches toward the $J/ψ$ production mechanism, are compared with experimental results and show reasonable agreement within uncertainties.