cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.68163.v1/t127
title: "Table 127" of "Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector"

description: Expected CLs in bCa_low SR for the $\tilde t_1\to b\chi^\pm_1$ scenario with $m_{\chi^\pm_1}=m_{\chi^0_1}+20$ GeV.
description: CERN-LHC. The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.
DOI: 10.17182/hepdata.68163.v1/t128
title: "Table 128" of "Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector"

description: Expected CLs in bCb_med1 SR for the $\tilde t_1\to b\chi^\pm_1$ scenario with $m_{\chi^\pm_1}=m_{\chi^0_1}+20$ GeV.
description: CERN-LHC. The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.
DOI: 10.17182/hepdata.68163.v1/t129
title: "Table 129" of "Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector"

description: Expected CLs in bCb_high SR for the $\tilde t_1\to b\chi^\pm_1$ scenario with $m_{\chi^\pm_1}=m_{\chi^0_1}+20$ GeV.
description: CERN-LHC. The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.
DOI: 10.17182/hepdata.68163.v1/t130
title: "Table 130" of "Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector"

description: Expected CLs in 3-body SR for the 3-body scenario ($\tilde t_1\to b W\chi^0_1$).
description: CERN-LHC. The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.
DOI: 10.17182/hepdata.68163.v1/t131
title: "Table 131" of "Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=$ 8 TeV pp collisions with the ATLAS detector"

description: Expected CLs in tNbC_mix SR for the mixed scenario (50% $\tilde t_1\to t\chi^0_1$, 50% $\tilde t_1\to b\chi^\pm_1$).
description: CERN-LHC. The results of a search for top squark (stop) pair production in final states with one isolated lepton, jets, and missing transverse momentum are reported. The analysis is performed with proton-proton collision data at $\sqrt{s}=$ 8 TeV collected with the ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of 20 fb$^{-1}$. The lightest supersymmetric particle (LSP) is taken to be the lightest neutralino which only interacts weakly and is assumed to be stable. The stop decay scenarios considered are those to a top quark and the LSP as well as to a bottom quark and the lightest chargino, where the chargino decays to the LSP by emitting a W boson. A wide range of scenarios with different mass splittings between the stop, the lightest neutralino and the lightest chargino are considered, including cases where the W bosons or the top quarks are off-shell. Decay scenarios involving the heavier charginos and neutralinos are addressed using a set of phenomenological models of supersymmetry. No significant excess over the Standard Model prediction is observed. A stop with a mass between 210 and 640 GeV decaying directly to a top quark and a massless LSP is excluded at 95% confidence level, and in models where the mass of the lightest chargino is twice that of the LSP, stops are excluded at 95% confidence level up to a mass of 500 GeV for an LSP mass in the range of 100 to 150 GeV. Stringent exclusion limits are also derived for all other considered stop decay scenarios, and generic upper limits are set on the visible cross-section for processes beyond the Standard Model.
DOI: 10.17182/hepdata.68361.v1/t1
title: "Table 1" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: dNdeta CL1.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t2
title: "Table 2" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: dNdeta V0M.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t3
title: "Table 3" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: dNdeta V0A.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t4
title: "Table 4" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: dNdeta ZNA.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t5
title: "Table 5" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb CL1.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t6
title: "Table 6" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb V0M.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t8
title: "Table 8" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb ZNA.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t10
title: "Table 10" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb hybrid mult.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t7
title: "Table 7" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb V0A.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.17182/hepdata.68361.v1/t9
title: "Table 9" of "Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV"

description: QpPb hybrid Pb-side.
description: CERN-LHC. We report measurements of the primary charged particle pseudorapidity
density and transverse momentum distributions in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV,
and investigate their correlation with experimental observables sensitive to the centrality
of the collision.

Modified 21 MAY 2015 by alice-publications@cern.ch.
In fig.16 only the systematic uncertainty for minimum bias was plotted.
Now, the uncertainty from the centrality selection was added.
DOI: 10.34740/kaggle/dsv/13612522
title: Peer-to-Peer Boliviano (BOB) Exchange Data
DOI: 10.17182/hepdata.68382.v1/t1
title: "Table 1" of "A study of tau decays involving eta and omega mesons."

description: $\pi^+\pi^-\pi^0$ mass distribution (two entries per event) in the $\pi^{\pm}\pi^+\pi^-\pi^0$ final state for the one-photon sample. The bin size has been chosen to display the detailed shape of the $\omega$ peak. The non-resonant contribution is represented by a simple polynomial. Non-$\tau$ background has been subtracted.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. The 132 pb$^{-1}$ of data collected by ALEPH from 1991 to 1994 have been used to analyze $\eta$ and $\omega$ production in $\tau$ decays. The following branching fractions have been measured:
$$\begin{eqnarray}
B(\tau^-\to\nu_{\tau}\omega h^-) = (1.91 \pm 0.07 \pm 0.06) \times 10^{-2},\\
B(\tau^-\to\nu_{\tau}\omega h^-\pi^0) = (4.3 \pm 0.6 \pm 0.5) \times 10^{-3},\\
B(\tau^-\to\nu_{\tau}\eta K^-) = (2.9^{+1.3}_{-1.2} \pm 0.7) \times 10^{-4},\\
B(\tau^-\to\nu_{\tau}\eta h^-\pi^0) = (1.8 \pm 0.4 \pm 0.2) \times 10^{-3}
\end{eqnarray}$$
and the 95% C.L. limit $B(\tau^-\to\nu_{\tau}\eta\pi^-) &lt; 6.2 \times 10^{-4}$ has been obtained. The $\omega\pi^-$ and $\eta\pi^-\pi^0$ rates and dynamics are found in agreement with the predictions made from $e^+e^-$ annihilation data with the help of isospin invariance (CVC).

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68382.v1/t2
title: "Table 2" of "A study of tau decays involving eta and omega mesons."

description: $\pi^+\pi^-\pi^0$ mass distributions (two entries per event) in the $\pi^{\pm}\pi^+\pi^-\pi^0$ final state for the two-photon sample. The bin size has been chosen to display the detailed shape of the $\omega$ peak. The non-resonant contribution is represented by a simple polynomial. Non-$\tau$ background has been subtracted.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. The 132 pb$^{-1}$ of data collected by ALEPH from 1991 to 1994 have been used to analyze $\eta$ and $\omega$ production in $\tau$ decays. The following branching fractions have been measured:
$$\begin{eqnarray}
B(\tau^-\to\nu_{\tau}\omega h^-) = (1.91 \pm 0.07 \pm 0.06) \times 10^{-2},\\
B(\tau^-\to\nu_{\tau}\omega h^-\pi^0) = (4.3 \pm 0.6 \pm 0.5) \times 10^{-3},\\
B(\tau^-\to\nu_{\tau}\eta K^-) = (2.9^{+1.3}_{-1.2} \pm 0.7) \times 10^{-4},\\
B(\tau^-\to\nu_{\tau}\eta h^-\pi^0) = (1.8 \pm 0.4 \pm 0.2) \times 10^{-3}
\end{eqnarray}$$
and the 95% C.L. limit $B(\tau^-\to\nu_{\tau}\eta\pi^-) &lt; 6.2 \times 10^{-4}$ has been obtained. The $\omega\pi^-$ and $\eta\pi^-\pi^0$ rates and dynamics are found in agreement with the predictions made from $e^+e^-$ annihilation data with the help of isospin invariance (CVC).

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68382.v1/t3
title: "Table 3" of "A study of tau decays involving eta and omega mesons."

description: Background-subtracted $\omega\pi$ mass spectrum for the data presented here, plotted as black dots.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. The 132 pb$^{-1}$ of data collected by ALEPH from 1991 to 1994 have been used to analyze $\eta$ and $\omega$ production in $\tau$ decays. The following branching fractions have been measured:
$$\begin{eqnarray}
B(\tau^-\to\nu_{\tau}\omega h^-) = (1.91 \pm 0.07 \pm 0.06) \times 10^{-2},\\
B(\tau^-\to\nu_{\tau}\omega h^-\pi^0) = (4.3 \pm 0.6 \pm 0.5) \times 10^{-3},\\
B(\tau^-\to\nu_{\tau}\eta K^-) = (2.9^{+1.3}_{-1.2} \pm 0.7) \times 10^{-4},\\
B(\tau^-\to\nu_{\tau}\eta h^-\pi^0) = (1.8 \pm 0.4 \pm 0.2) \times 10^{-3}
\end{eqnarray}$$
and the 95% C.L. limit $B(\tau^-\to\nu_{\tau}\eta\pi^-) &lt; 6.2 \times 10^{-4}$ has been obtained. The $\omega\pi^-$ and $\eta\pi^-\pi^0$ rates and dynamics are found in agreement with the predictions made from $e^+e^-$ annihilation data with the help of isospin invariance (CVC).

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68382.v1/t4
title: "Table 4" of "A study of tau decays involving eta and omega mesons."

description: Background-subtracted $\omega\pi$ mass spectrum for the data from the ND experiment [S.I. Dolinski et al., Phys. Rep. 202 (1991) 99], plotted as open circles.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. The 132 pb$^{-1}$ of data collected by ALEPH from 1991 to 1994 have been used to analyze $\eta$ and $\omega$ production in $\tau$ decays. The following branching fractions have been measured:
$$\begin{eqnarray}
B(\tau^-\to\nu_{\tau}\omega h^-) = (1.91 \pm 0.07 \pm 0.06) \times 10^{-2},\\
B(\tau^-\to\nu_{\tau}\omega h^-\pi^0) = (4.3 \pm 0.6 \pm 0.5) \times 10^{-3},\\
B(\tau^-\to\nu_{\tau}\eta K^-) = (2.9^{+1.3}_{-1.2} \pm 0.7) \times 10^{-4},\\
B(\tau^-\to\nu_{\tau}\eta h^-\pi^0) = (1.8 \pm 0.4 \pm 0.2) \times 10^{-3}
\end{eqnarray}$$
and the 95% C.L. limit $B(\tau^-\to\nu_{\tau}\eta\pi^-) &lt; 6.2 \times 10^{-4}$ has been obtained. The $\omega\pi^-$ and $\eta\pi^-\pi^0$ rates and dynamics are found in agreement with the predictions made from $e^+e^-$ annihilation data with the help of isospin invariance (CVC).

These numbers have been read from the plots in the paper.
DOI: 10.17182/hepdata.68382.v1/t5
title: "Table 5" of "A study of tau decays involving eta and omega mesons."

description: Background-subtracted $\omega\pi$ mass spectrum for the data from the DM2 experiment [D. Bisello et al., Nucl. Phys. B 21 (Proc. Supp.) (1991) 111], plotted as open squares.

The error has been set to zero if it is smaller than the point size.
description: CERN-LEP. The 132 pb$^{-1}$ of data collected by ALEPH from 1991 to 1994 have been used to analyze $\eta$ and $\omega$ production in $\tau$ decays. The following branching fractions have been measured:
$$\begin{eqnarray}
B(\tau^-\to\nu_{\tau}\omega h^-) = (1.91 \pm 0.07 \pm 0.06) \times 10^{-2},\\
B(\tau^-\to\nu_{\tau}\omega h^-\pi^0) = (4.3 \pm 0.6 \pm 0.5) \times 10^{-3},\\
B(\tau^-\to\nu_{\tau}\eta K^-) = (2.9^{+1.3}_{-1.2} \pm 0.7) \times 10^{-4},\\
B(\tau^-\to\nu_{\tau}\eta h^-\pi^0) = (1.8 \pm 0.4 \pm 0.2) \times 10^{-3}
\end{eqnarray}$$
and the 95% C.L. limit $B(\tau^-\to\nu_{\tau}\eta\pi^-) &lt; 6.2 \times 10^{-4}$ has been obtained. The $\omega\pi^-$ and $\eta\pi^-\pi^0$ rates and dynamics are found in agreement with the predictions made from $e^+e^-$ annihilation data with the help of isospin invariance (CVC).

These numbers have been read from the plots in the paper.