cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.126972.v1/t15
title: "Table_T15" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.819
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t16
title: "Table_T16" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.906
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t17
title: "Table_T17" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.966
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126972.v1/t18
title: "Table_T18" of "Threshold π0 photoproduction on transverse polarised protons at MAMI"

description: Target asymmetry T for c.m. cos(Theta_pi0)= -0.996
description: A2 Collaboration at MAMI.
Polarisation-dependent differential cross sections $\sigma_T$ associated
with the target asymmetry T have been measured for the reaction $\gamma p \to \pi^0 p$
from threshold to photon energies of 190 MeV. We present here the results for
the target asymmetry T that have been obtained by dividing $\sigma_T$ to our
previous data for the unpolarised differential cross sections. Global systematic
uncertainties arise from the determination of the photon flux (3%)
and the overall detector and electronics performance (3%). For the target density
the total uncertainty of 6% is given by the effective target length (2.0±0.1cm) and
the packing fraction (61%±2%). The target polarisation has been determined with an
accuracy of 2%. Quadratic addition of the individual contributions
results in global uncertainties of about 8%. The data were obtained using
a frozen-spin butanol target with the Crystal Ball/TAPS detector set-up and
the Glasgow photon tagging system at the Mainz Microtron MAMI.
DOI: 10.17182/hepdata.126990.v1/t1
title: "Table 1" of "Study of $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured values of $R_{D_s^+/\pi^+}$, $R_{D_s^{*+}/\pi^+}$, $R_{D_s^{*+}/D_s^+}$ ratios of branching fractions, fraction of transverse polarization $\Gamma_{\pm\pm}/\Gamma$ with their statistical uncertainties and full breakdown of systematic uncertainties. Predictions of various theory calculations are also shown with their uncertainties where available, as well as the estimates based on similar decays of light $B$ mesons.
description: A study of the $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays
using 139\,fb$^{-1}$ of integrated luminosity collected with the ATLAS detector
from $\sqrt{s} = 13$\,TeV $pp$ collisions at the LHC is presented.
The ratios of the branching fractions of the two decays to the
branching fraction of $B_c^+\to J/\psi \pi^+$ decay channel are measured:
$\mathcal B(B_c^+\to J/\psi D_s^+)/\mathcal B(B_c^+\to J/\psi \pi^+) = 2.76\pm 0.33\pm 0.29\pm 0.16$,
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi \pi^+) = 5.33\pm0.61\pm 0.67\pm 0.32$.
Here the first error is statistical, the second is systematic, and the third is
due to uncertainty on the $D_s^+\to\phi(K^+ K^-)\pi^+$ decay branching fraction.
The ratio between the branching fractions of the two decays is found to be
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi D_s^+) = 1.93\pm0.24 \pm 0.09$.
For the $B_c^+\to J/\psi D_s^{*+}$ decay, the transverse polarisation fraction, $\Gamma_{\pm\pm}/\Gamma$, is measured
to be $0.70\pm0.10\pm 0.04$. The precision of the measurements exceeds that of
all previous studies of these decays.
DOI: 10.17182/hepdata.126990.v1/t3
title: "Table 3" of "Study of $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Parameters of the $B_c^+\to J/\psi \pi^+$ signal obtained with the unbinned extended maximum-likelihood fit. Only the statistical uncertainties are included. No efficiency correction is applied to the signal yield.
description: A study of the $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays
using 139\,fb$^{-1}$ of integrated luminosity collected with the ATLAS detector
from $\sqrt{s} = 13$\,TeV $pp$ collisions at the LHC is presented.
The ratios of the branching fractions of the two decays to the
branching fraction of $B_c^+\to J/\psi \pi^+$ decay channel are measured:
$\mathcal B(B_c^+\to J/\psi D_s^+)/\mathcal B(B_c^+\to J/\psi \pi^+) = 2.76\pm 0.33\pm 0.29\pm 0.16$,
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi \pi^+) = 5.33\pm0.61\pm 0.67\pm 0.32$.
Here the first error is statistical, the second is systematic, and the third is
due to uncertainty on the $D_s^+\to\phi(K^+ K^-)\pi^+$ decay branching fraction.
The ratio between the branching fractions of the two decays is found to be
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi D_s^+) = 1.93\pm0.24 \pm 0.09$.
For the $B_c^+\to J/\psi D_s^{*+}$ decay, the transverse polarisation fraction, $\Gamma_{\pm\pm}/\Gamma$, is measured
to be $0.70\pm0.10\pm 0.04$. The precision of the measurements exceeds that of
all previous studies of these decays.
DOI: 10.17182/hepdata.126990.v1/t4
title: "Table 4" of "Study of $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Summary of the total efficiencies. Quoted uncertainties correspond to statistical uncertainties of the simulated samples used. For the $B_c^+\to J/\psi \pi^+$ channel, the efficiency $\epsilon_{B_c^+\to J/\psi \pi^+}$ entering the equations for $R_{D_s^{(*)+}/\pi^+}$ is shown, while the efficiency for the full dataset is not defined.
description: A study of the $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays
using 139\,fb$^{-1}$ of integrated luminosity collected with the ATLAS detector
from $\sqrt{s} = 13$\,TeV $pp$ collisions at the LHC is presented.
The ratios of the branching fractions of the two decays to the
branching fraction of $B_c^+\to J/\psi \pi^+$ decay channel are measured:
$\mathcal B(B_c^+\to J/\psi D_s^+)/\mathcal B(B_c^+\to J/\psi \pi^+) = 2.76\pm 0.33\pm 0.29\pm 0.16$,
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi \pi^+) = 5.33\pm0.61\pm 0.67\pm 0.32$.
Here the first error is statistical, the second is systematic, and the third is
due to uncertainty on the $D_s^+\to\phi(K^+ K^-)\pi^+$ decay branching fraction.
The ratio between the branching fractions of the two decays is found to be
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi D_s^+) = 1.93\pm0.24 \pm 0.09$.
For the $B_c^+\to J/\psi D_s^{*+}$ decay, the transverse polarisation fraction, $\Gamma_{\pm\pm}/\Gamma$, is measured
to be $0.70\pm0.10\pm 0.04$. The precision of the measurements exceeds that of
all previous studies of these decays.
DOI: 10.17182/hepdata.127138.v1/t1
title: "tHb mass in the signal region" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: Reconstructed W′ boson mass distributions in the tHb signal region.
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.17182/hepdata.127138.v1/t2
title: "tZb mass in the signal region" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: Reconstructed W′ boson mass distributions in the tZb signal region.
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.17182/hepdata.127138.v1/t3
title: "center VLQ mass limits" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits are shown for the center VLQ mass range.
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.25549/vercoutere-ouc110610142
title: Partially nude reclining woman plus word salad

description: One partially nude orange female with black hair and red panties reclining against blankets of green, tan, and brown; a small word salad is printed in pencil in the lower right corner; remainder of page is unpainted. See description of 347 for OT notes.
DOI: 10.17182/hepdata.126990.v1/t2
title: "Table 2" of "Study of $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Parameters of the $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ signals obtained with the unbinned extended maximum-likelihood fit to the data. Only the statistical uncertainties are included. No acceptance or efficiency corrections are applied to the signal yields.
description: A study of the $B_c^+\to J/\psi D_s^+$ and $B_c^+\to J/\psi D_s^{*+}$ decays
using 139\,fb$^{-1}$ of integrated luminosity collected with the ATLAS detector
from $\sqrt{s} = 13$\,TeV $pp$ collisions at the LHC is presented.
The ratios of the branching fractions of the two decays to the
branching fraction of $B_c^+\to J/\psi \pi^+$ decay channel are measured:
$\mathcal B(B_c^+\to J/\psi D_s^+)/\mathcal B(B_c^+\to J/\psi \pi^+) = 2.76\pm 0.33\pm 0.29\pm 0.16$,
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi \pi^+) = 5.33\pm0.61\pm 0.67\pm 0.32$.
Here the first error is statistical, the second is systematic, and the third is
due to uncertainty on the $D_s^+\to\phi(K^+ K^-)\pi^+$ decay branching fraction.
The ratio between the branching fractions of the two decays is found to be
$\mathcal B(B_c^+\to J/\psi D_s^{*+})/\mathcal B(B_c^+\to J/\psi D_s^+) = 1.93\pm0.24 \pm 0.09$.
For the $B_c^+\to J/\psi D_s^{*+}$ decay, the transverse polarisation fraction, $\Gamma_{\pm\pm}/\Gamma$, is measured
to be $0.70\pm0.10\pm 0.04$. The precision of the measurements exceeds that of
all previous studies of these decays.
DOI: 10.17182/hepdata.127138.v1/t4
title: "high VLQ mass limits" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits are shown for the high VLQ mass range.
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.17182/hepdata.127138.v1/t6
title: "Generalized Expected tB,bT limits" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: Expected 95% CL limits for generalized hypotheses varying the fraction of tB (F(VLQ=B)) and bT (F(VLQ=T)) from the W′ decay
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.17182/hepdata.127138.v1/t7
title: "Generalized Expected qH,qZ limits" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: Expected 95% CL limits for generalized hypotheses varying the VLQ branching fraction to qH and qZ
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.
DOI: 10.17182/hepdata.127138.v1/t5
title: "low VLQ mass limits" of "Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state at $\sqrt{s}$ = 13 TeV"

description: The W' boson 95% CL limits on the product of cross section and branching fraction. The expected and observed limits are shown for the low VLQ mass range.
description: A search is presented for a heavy $\mathrm{W\prime}$ boson resonance decaying to a $\mathrm{B}$ or $\mathrm{T}$ vector-like quark and a $\mathrm{t}$ or a $\mathrm{b}$ quark, respectively. The analysis is performed using proton-proton collisions collected with the CMS detector at the LHC. The data correspond to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ at a center-of-mass energy of 13 TeV. Both decay channels result in a signature with a $\mathrm{t}$ quark, a Higgs or $\mathrm{Z}$ boson, and a $\mathrm{b}$ quark, each produced with a significant Lorentz boost. The all-hadronic decays of the Higgs or $\mathrm{Z}$ boson and of the $\mathrm{t}$ quark are selected using jet substructure techniques to reduce standard model backgrounds, resulting in a distinct three-jet $\mathrm{W\prime}$ boson decay signature. No significant deviation in data with respect to the standard model background prediction is observed. Upper limits are set at 95\% confidence level on the product of the $\mathrm{W\prime}$ boson cross section and the final state branching fraction. A $\mathrm{W\prime}$ boson with a mass below 3.2 TeV is excluded, given the benchmark model assumption of democratic branching fractions. In addition, limits are set based on generalizations of these assumptions. These are the most sensitive limits to date for this final state.