cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95664.v2/t67
title: "X-section U.L 3" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: The observed upper limits on signal cross section corresponding to the best expected signal region in each mass point for squark-pair production with a one-step decay via an intermediate chargino.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t68
title: "X-section U.L 4" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: The observed upper limits on signal cross section corresponding to the best expected signal region in each mass point for squark-pair production with a one-step decay via an intermediate chargino. The neutralino mass is fixed at 60 GeV and exclusion limits are given for mass difference ratio, $X$, as a function of the squark mass.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t69
title: "X-section U.L 5" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: The observed upper limits on signal cross section corresponding to the best expected signal region in each mass point for gluino-pair production with a one-step decay via an intermediate chargino.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t70
title: "X-section U.L 6" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: The observed upper limits on signal cross section corresponding to the best expected signal region in each mass point for gluino-pair production with a one-step decay via an intermediate chargino. The neutralino mass is fixed at 60~GeV and exclusio limits are given for mass difference ratio, $X$, as a function of the gluino mass.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t71
title: "Cut flow 1" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: Cut-flow for model-independent search regions targeting squarks for SS direct model points. Expected yields are normalized to a luminosity of 139 fb$^{-1}$.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t72
title: "Cut flow 2" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: Cut-flow for model-independent search regions targeting gluinos for GG direct model points. Expected yields are normalized to a luminosity of 139 fb$^{-1}$.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t74
title: "Cut flow 4" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: Cut-flow for BDT search regions targeting gluinos in models with one-step decays. Expected yields are normalized to a luminosity of 139 $fb^{-1}$.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t73
title: "Cut flow 3" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: Cut-flow for model-independent search regions targeting squarks and gluinos in models with one-step decay. Expected yields are normalized to a luminosity of 139 $fb^{-1}$.
description: No data abstract available.
DOI: 10.17182/hepdata.95664.v2/t75
title: "Cut flow 5" of "Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb$^{-1}$ of $\sqrt{s}$ =13 TeV $pp$ collision data with the ATLAS detector"

description: Cut-flow for BDT search regions targeting gluinos in models with direct decays. Expected yields are normalized to a luminosity of 139 $fb^{-1}$.
description: No data abstract available.
DOI: 10.17182/hepdata.95676.v1/t1
title: "Table 1" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Results of the fit to data. Statistical uncertainties are obtained from the increase in $-\log{\mathcal{L}}$ by 0.5.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events. The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018. To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques. The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions. When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, 
the following values are obtained: $\phi_{\mathrm{s}} = -21 \pm 45\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1073 \pm 0.0097\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v1/t2
title: "Table 2" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Values of parameter obtained combining the 13 TeV results with those obtained at 8 TeV. Uncertainties are both statistical and systematic.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events. The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018. To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques. The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions. When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, 
the following values are obtained: $\phi_{\mathrm{s}} = -21 \pm 45\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1073 \pm 0.0097\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v1/t3
title: "Table 3" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Statistical error correlation matrix of the physics parameters of interest, as obtained from the fit to data at 13 TeV.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events. The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018. To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques. The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions. When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, 
the following values are obtained: $\phi_{\mathrm{s}} = -21 \pm 45\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1073 \pm 0.0097\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v1/t4
title: "Table 4" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Error correlation matrix physics parameters of interest for the 8+13 TeV combination.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events. The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018. To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques. The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions. When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, 
the following values are obtained: $\phi_{\mathrm{s}} = -21 \pm 45\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1073 \pm 0.0097\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v2/t1
title: "Table 1" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Results of the fit to the data at 13 TeV. Statistical uncertainties are obtained from the increase in $-\log{\mathcal{L}}$ by 0.5.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events.
The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018.
To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques.
The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions.
When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, the following values are obtained:
$\phi_{\mathrm{s}} = -21 \pm 44\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1032 \pm 0.0095\,\text{(stat)} \pm 0.0048\,\text{(syst)}\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v2/t2
title: "Table 2" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Values of parameter obtained combining the 13 TeV results with those obtained by CMS at 8 TeV.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events.
The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018.
To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques.
The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions.
When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, the following values are obtained:
$\phi_{\mathrm{s}} = -21 \pm 44\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1032 \pm 0.0095\,\text{(stat)} \pm 0.0048\,\text{(syst)}\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v2/t3
title: "Table 3" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Statistical correlation matrix of the physics parameters of interest, as obtained from the fit to data at 13 TeV.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events.
The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018.
To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques.
The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions.
When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, the following values are obtained:
$\phi_{\mathrm{s}} = -21 \pm 44\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1032 \pm 0.0095\,\text{(stat)} \pm 0.0048\,\text{(syst)}\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95676.v2/t4
title: "Table 4" of "Measurement of the $CP$ violating phase $\phi_{\text{s}}$ in the $\mathrm{B}_s \to \mathrm{J}/\psi\,\phi(1020) \to \mu^+\mu^-\,\mathrm{K}^+\mathrm{K}^-$ channel in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$"

description: Total correlation matrix of the physics parameters of interest for the 8+13 TeV combination.
description: The CP-violating weak phase $\phi_{\mathrm{s}}$ and the decay width 
difference $\Delta\Gamma_{\mathrm{s}}$ between the light and heavy 
$\mathrm{B}^0_\mathrm{s}$ mass eigenstates are measured with the CMS 
detector at the LHC in a sample of $48\,500$ reconstructed
$\mathrm{B}^0_\mathrm{s}\to\mathrm{J /\psi}\,\mathrm{\phi(1020)} \to \mathrm{\mu^+}\mathrm{\mu^-}\,\mathrm{K^+}\mathrm{K^-}$ 
events.
The measurement is based on a data sample corresponding to 
an integrated luminosity of $96.4\,\text{fb}^{-1}$, collected in 
proton-proton collisions at $\sqrt{s} = 13\,\text{TeV}$ 
in 2017--2018.
To extract the values of $\phi_{\mathrm{s}}$ and 
$\Delta\Gamma_{\mathrm{s}}$, a time-dependent and flavor-tagged 
angular analysis of the $\mathrm{\mu^+}\mathrm{\mu^-}\mathrm{K^+}\mathrm{K^-}$ 
final state is performed. The analysis employs a dedicated tagging 
trigger and a novel opposite-side muon flavor tagger based on machine 
learning techniques.
The measurement yields 
$\phi_{\mathrm{s}} = -11 \pm 50\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$ 
and 
$\Delta\Gamma_{\mathrm{s}} = 0.114 \pm 0.014\,\text{(stat)} \pm 0.007\,\text{(syst)}\,\text{ps}^{-1}$, 
in agreement with the standard model predictions.
When combined with the 
previous CMS measurement at $\sqrt{s} = 8\,\text{TeV}$, the following values are obtained:
$\phi_{\mathrm{s}} = -21 \pm 44\,\text{(stat)} \pm 10\,\text{(syst)}\,\text{mrad}$, 
$\Delta\Gamma_{\mathrm{s}} = 0.1032 \pm 0.0095\,\text{(stat)} \pm 0.0048\,\text{(syst)}\,\text{ps}^{-1}$, 
a significant improvement over the 8 TeV result.
DOI: 10.17182/hepdata.95683.v1/t1
title: "Overview" of "Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC"

description: <b>- - - - - - - - Overview of HEPData Record - - - - - - - -</b> <br><br>
<b>Exclusion contours:</b>

Stop to bottom quark and chargino exclusion contour (Obs.)
Stop to bottom quark and chargino exclusion contour (Exp.)
Stop to higgsino LSP exclusion contour (Obs.)
Stop to higgsino LSP exclusion contour (Exp.)
Stop to top quark and neutralino exclusion contour (Obs.)
Stop to top quark and neutralino exclusion contour (Exp.)

<b>Upper limits:</b>

Obs Xsection upper limit in stop to bottom quark and chargino
Obs Xsection upper limit in higgsino LSP
Exp Xsection upper limit in stop to bottom quark and chargino
Exp Xsection upper limit in higgsino LSP

<b>Kinematic distributions:</b>

SR_yields

<b>Cut flows:</b>

cutflow

<b>Acceptance and efficiencies:</b>
As explained in the twiki.

 <b>stbchi_6je4be:</b> stbchi_Acc_6je4be stbchi_Eff_6je4be
 <b>stbchi_7je4be:</b> stbchi_Acc_7je4be stbchi_Eff_7je4be
 <b>stbchi_8je4be:</b> stbchi_Acc_8je4be stbchi_Eff_8je4be
 <b>stbchi_9ji4be:</b> stbchi_Acc_9ji4be stbchi_Eff_9ji4be
 <b>stbchi_6je5bi:</b> stbchi_Acc_6je5bi stbchi_Eff_6je5bi
 <b>stbchi_7je5bi:</b> stbchi_Acc_7je5bi stbchi_Eff_7je5bi
 <b>stbchi_8je5bi:</b> stbchi_Acc_8je5bi stbchi_Eff_8je5bi
 <b>stbchi_9ji5bi:</b> stbchi_Acc_9ji5bi stbchi_Eff_9ji5bi
 <b>stbchi_8ji5bi:</b> stbchi_Acc_8ji5bi stbchi_Eff_8ji5bi
 <b>sttN_6je4be:</b> sttN_Acc_6je4be sttN_Eff_6je4be
 <b>sttN_7je4be:</b> sttN_Acc_7je4be sttN_Eff_7je4be
 <b>sttN_8je4be:</b> sttN_Acc_8je4be sttN_Eff_8je4be
 <b>sttN_9ji4be:</b> sttN_Acc_9ji4be sttN_Eff_9ji4be
 <b>sttN_6je5bi:</b> sttN_Acc_6je5bi sttN_Eff_6je5bi
 <b>sttN_7je5bi:</b> sttN_Acc_7je5bi sttN_Eff_7je5bi
 <b>sttN_8je5bi:</b> sttN_Acc_8je5bi sttN_Eff_8je5bi
 <b>sttN_9ji5bi:</b> sttN_Acc_9ji5bi sttN_Eff_9ji5bi
 <b>sttN_8ji5bi:</b> sttN_Acc_8ji5bi sttN_Eff_8ji5bi

<b>Truth Code snippets</b> and <b>SLHA files are available under "Resources" (purple button on the left)</b>
description: No data abstract available.
DOI: 10.17182/hepdata.95683.v1/t3
title: "stbchionly_exp" of "Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC"

description: The expected exclusion contour at 95% CL as a function of the $\it{m}_{\tilde{\chi}^{\pm}_{1}}$ vs. $\it{m}_{\tilde{t}}$. Masses that are within the contour are excluded. Limits are shown for $B(\tilde{t} \rightarrow b \chi^{+}_{1})$ equal to unity.
description: No data abstract available.
DOI: 10.17182/hepdata.95683.v1/t4
title: "stbchi_obs" of "Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC"

description: The observed exclusion contour at 95% CL as a function of the $\it{m}_{\tilde{\chi}^{0}_{1}}$ vs. $\it{m}_{\tilde{t}}$. Masses that are within the contours are excluded. Limits are shown in the case of a higgsino LSP. The results are constrained by the kinematic limits of the top-squark decay into a chargino and a bottom quark (upper diagonal line) and into a neutralino and a top quark (lower diagonal line), respectively.
description: No data abstract available.
DOI: 10.17182/hepdata.95683.v1/t10
title: "stbchionly_xSecUL_exp" of "Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC"

description: Expected model-dependent upper limit on the cross section for the $(\tilde{t},\tilde{\chi}^{\pm}_{1})$ signal grid. Limits are shown for $B(\tilde{t} \rightarrow b \chi^{+}_{1})$ equal to unity.
description: No data abstract available.
DOI: 10.17182/hepdata.95683.v1/t2
title: "stbchionly_obs" of "Search for phenomena beyond the Standard Model in events with large $b$-jet multiplicity using the ATLAS detector at the LHC"

description: The observed exclusion contour at 95% CL as a function of the $\it{m}_{\tilde{\chi}^{\pm}_{1}}$ vs. $\it{m}_{\tilde{t}}$. Masses that are within the contours are excluded. Limits are shown for $B(\tilde{t} \rightarrow b \chi^{+}_{1})$ equal to unity.
description: No data abstract available.