cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93068.v1/t60
title: "Table 60" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Covariance of the differential charge ratio as a function of the particle-level top quark $p_\textrm{T}$
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t61
title: "Table 61" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Differential charge ratio as a function of the particle-level top quark rapidity
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t62
title: "Table 62" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Covariance of the differential charge ratio as a function of the particle-level top quark rapidity
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t63
title: "Table 63" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Differential charge ratio as a function of the particle-level charged lepton $p_\textrm{T}$
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t64
title: "Table 64" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Covariance of the differential charge ratio as a function of the particle-level charged lepton $p_\textrm{T}$
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t65
title: "Table 65" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Differential charge ratio as a function of the particle-level charged lepton rapidity
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t66
title: "Table 66" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Covariance of the differential charge ratio as a function of the particle-level charged lepton rapidity
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t67
title: "Table 67" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Differential charge ratio as a function of the particle-level W boson $p_\textrm{T}$
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t68
title: "Table 68" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Covariance of the differential charge ratio as a function of the particle-level W boson $p_\textrm{T}$
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93068.v1/t69
title: "Table 69" of "Measurement of differential cross sections and charge ratios for $t$-channel single top quark production in proton-proton collisions at $\sqrt{s}=$ 13 TeV"

description: Top quark spin asymmetry at the parton level in the muon and electron channel and their combination
description: A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of $13~\rm{TeV}$ by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of $35.9~\rm{fb}^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_{\rm{T}}$), rapidity, and polarisation angle, the charged lepton $p_{\rm{T}}$ and rapidity, and the $p_{\rm{T}}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be $0.440 \pm 0.070$, in agreement with the standard model prediction.
DOI: 10.17182/hepdata.93069.v1/t1
title: "Table 1" of "Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic couplings"

description: The measured EWK Zgamma+2j fiducial cross section. The uncertainty is the combined stastical uncertianty and the systematic uncertainty including experimental and theortical sources
description: CERN-LHC. Measurement of the cross section for electroweak production and
constraints on anomalous quartic couplings from events with a Z boson
and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV.
The Z boson candidates are selected through their decay into a pair of electrons or muons.
The process of interest, electroweak Z gamma jj production, is isolated by selecting
events with a large dijet mass and a large pseudorapidity gap between the two jets.
The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass
energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1.
The observed significance of the signal is 3.9 standard deviations, where a significance of
5.2 standard deviations is expected in the standard model predictions.
The results are combined with previously published CMS results based on sqrt(s)=8 TeV data,
which leads to an observed (expected) significance of 4.7 (5.5) standard deviations.
The measured value of the fiducial cross section for the signal is reported. 
Bounds are given on quartic vector boson interactions in the framework of dimension-8
effective field theory operators at 95% confidence level.
The fiducial region is defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt;20 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
- leptons are dressed with photons whose DeltaR(l,photon)&lt;0.1
Selections for aQGC limits are defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt; 100 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
DOI: 10.17182/hepdata.93069.v1/t2
title: "Table 2" of "Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic couplings"

description: The measured combined QCD-induced and EWK Zgamma+2j fiducial cross section. The uncertainty is the combined stastical uncertianty and the systematic uncertainty including experimental and theortical sources
description: CERN-LHC. Measurement of the cross section for electroweak production and
constraints on anomalous quartic couplings from events with a Z boson
and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV.
The Z boson candidates are selected through their decay into a pair of electrons or muons.
The process of interest, electroweak Z gamma jj production, is isolated by selecting
events with a large dijet mass and a large pseudorapidity gap between the two jets.
The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass
energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1.
The observed significance of the signal is 3.9 standard deviations, where a significance of
5.2 standard deviations is expected in the standard model predictions.
The results are combined with previously published CMS results based on sqrt(s)=8 TeV data,
which leads to an observed (expected) significance of 4.7 (5.5) standard deviations.
The measured value of the fiducial cross section for the signal is reported. 
Bounds are given on quartic vector boson interactions in the framework of dimension-8
effective field theory operators at 95% confidence level.
The fiducial region is defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt;20 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
- leptons are dressed with photons whose DeltaR(l,photon)&lt;0.1
Selections for aQGC limits are defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt; 100 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
DOI: 10.17182/hepdata.93069.v1/t3
title: "Table 3" of "Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV and constraints on anomalous quartic couplings"

description: aQGC limits on effective field theory parameters in EWK Zgamma events
description: CERN-LHC. Measurement of the cross section for electroweak production and
constraints on anomalous quartic couplings from events with a Z boson
and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV.
The Z boson candidates are selected through their decay into a pair of electrons or muons.
The process of interest, electroweak Z gamma jj production, is isolated by selecting
events with a large dijet mass and a large pseudorapidity gap between the two jets.
The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass
energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1.
The observed significance of the signal is 3.9 standard deviations, where a significance of
5.2 standard deviations is expected in the standard model predictions.
The results are combined with previously published CMS results based on sqrt(s)=8 TeV data,
which leads to an observed (expected) significance of 4.7 (5.5) standard deviations.
The measured value of the fiducial cross section for the signal is reported. 
Bounds are given on quartic vector boson interactions in the framework of dimension-8
effective field theory operators at 95% confidence level.
The fiducial region is defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt;20 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
- leptons are dressed with photons whose DeltaR(l,photon)&lt;0.1
Selections for aQGC limits are defined as:
- ptl&gt;20 GeV(25 GeV) && |etaLepton|&lt;2.4(2.5) form muon(electron)
- third lepton veto
- 70 GeV &lt; Mll &lt; 110 GeV
- photon pT&gt; 100 GeV && |etaPhoton|&lt;1.442 or (|etaPhoton|&gt;1.566 && |etaPhoton|&lt;2.5) 
 for barrel and endcap
- ptjet&gt;30 GeV && |etaJet|&lt;4.7
- Mjj &gt; 500 GeV && |deltaetajj|&gt;2.5
- DeltaR(l,photon)&gt;0.7 && DeltaR(l,j)&gt;0.5 && Delta(photon,j)&gt;0.5 && DeltaR(j,j)&gt;0.5
DOI: 10.17182/hepdata.93070.v1/t1
title: "Table 1" of "Study of $\Upsilon$ production in $p$Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV"

description: $\Upsilon(1S)$ production cross-section in $p$Pb, as a function of $p_{T}$ and $y*$. The uncertainty is the sum in quadrature of the statistical and systematic components.
description: CERN-LHC. The production of $\Upsilon(nS)$ mesons ($n=1,2,3$) in $p$Pb and Pb$p$ collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{NN}}=8.16$ TeV is measured by the LHCb experiment, using a data sample corresponding to an integrated luminosity of 31.8 $nb^{-1}$. The $\Upsilon(nS)$ mesons are reconstructed through their decays into two opposite-sign muons. The measurements comprise the differential production cross-sections of the $\Upsilon(1S)$ and $\Upsilon(2S)$ states, their forward-to-backward ratios and nuclear modification factors, performed as a function of the transverse momentum p_{T} and rapidity in the nucleon-nucleon centre-of-mass frame $y^*$ of the $\Upsilon(nS)$ states, in the kinematic range $p_{T}&lt;25$ GeV$/c$ and $1.5