cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.115490.v1/t27
title: "Figure 15 (left)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross section as a function of the invariant mass of two b jets for the Z + &gt;= 2 b jet events
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.25549/vercoutere-ouc110610346
title: 2 19th century men plus word salad

description: One male with brown hair, side burns, and a moustache wearing a knee-length coat of blue, orange lapel, black arm, orange vest, brown pants and shoes standing with one arm resting on a table; magenta and purple chair on one side with a hanging round painting; a brown male head with brown hair above a purple desk top with brown books on top; remainder of the page is a word salad printed in purple on an unpainted background. See description of 347 for OT notes.
DOI: 10.17182/hepdata.115490.v1/t24
title: "Figure 13 (right)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized differential cross section as a function of the minimum angular separation between the Z boson and two b jets for the Z + &gt;= 2 b jet events
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.17182/hepdata.115490.v1/t29
title: "Figure 16 (left)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Differential cross section as a function of the invariant mass of the Z boson and two b jets for the Z + &gt;= 2 b jet events
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.17182/hepdata.115490.v1/t30
title: "Figure 16 (right)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized differential cross section as a function of invariant mass of the Z boson and two b jets for the Z + &gt;= 2 b jet events
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.17182/hepdata.115490.v1/t31
title: "Figure 17 (left)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of the cross section ratios as a function of the leading b jet transverse momentum
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.17182/hepdata.115511.v1/t1
title: "CL for 1SFH e Dirac model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 1SFH e Dirac model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t2
title: "CL for 1SFH e Majorana model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 1SFH e Majorana model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115490.v1/t28
title: "Figure 15 (right)" of "Measurement of the production cross section for Z + b jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized differential cross section as a function of the invariant mass of two b jets for the Z + &gt;= 2 b jet events
description: The measurements of the cross section of the \PZ boson, decaying to dielectrons or dimuons, in association with at least one bottom quark jet are performed with proton-proton collision data at $\sqrt{s}=$ 13\TeV. The data sample corresponds to an integrated luminosity of 137.1\fbinv, collected by the CMS experiment at the LHC. The integrated cross sections of \PZ~$+\geq$~1~\cPqb~jet\xspace and \PZ~$+\geq$~2~\cPqb~jets\xspace are reported for the electron, muon, and combined channels with full Run 2 data. The measured integrated cross sections are 6.52 $\pm$ 0.04 (stat) $\pm$ 0.40 (syst) $\pm$ 0.14 (theo) pb for \PZ~$+\geq$~1~\cPqb~jet\xspace and 0.65 $\pm$ 0.03 (stat) $\pm$ 0.07 (syst) $\pm$ 0.02 (theo) pb for \PZ~$+\geq$~2~\cPqb~jets\xspace. The differential cross section distributions are measured as a function of various kinematic observables that are useful for precision tests of the perturbative quantum chromodynamics predictions. The ratios of integrated and differential cross sections of \PZ~$+\geq$~2~\cPqb~jets\xspace and \PZ~$+\geq$~1~\cPqb~jet\xspace processes are also determined. The value of the integrated cross section ratio measured in the combined channel is 0.100 $\pm$ 0.005 (stat) $\pm$ 0.007 (syst) $\pm$ 0.003 (theo). All of the measurements are compared with predictions from Monte Carlo simulations.
DOI: 10.17182/hepdata.115511.v1/t3
title: "CL for 1SFH mu Dirac model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 1SFH mu Dirac model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t4
title: "CL for 1SFH mu Majorana model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 1SFH mu Majorana model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t5
title: "CL for 2QDH NH Dirac model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 2QDH NH Dirac model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t7
title: "CL for 2QDH IH Dirac model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 2QDH IH Dirac model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.25549/vercoutere-ouc110610369
title: Nude woman and nude man with apple tree plus word salad

description: One orange nude female with reddish brown hair standing next to a orange and brown nude male with brown hair and erect penis; area around figures is green with apples hanging from branches; remainder of the page is a word salad printed in red, green, blue, orange, black, blue, and purple on an unpainted background. See description of 347 for OT notes.
DOI: 10.17182/hepdata.115511.v1/t10
title: "Cutflow Data selection" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Cutflow for the six channels in data showing the number of events passing each successive signal selection for Majorana HNLs.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t12
title: "Vertexing uncertainty" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: The dominant signal uncertainty is due to differences in reconstruction of displaced vertices and tracks between data and MC. This is evaluated by comparing $K^{0}_{S} \rightarrow \pi^+\pi^-$ event yields in the VR and in MC produced with Pythia8.186 in bins of $p_\mathrm{T}$ and $r_\mathrm{DV}$. The data/MC ratio is normalized to the bin nearest the IP where the tracking and vertexing reconstruction algorithms are expected to be most robust. The symmetrized difference from 1.0 is applied to each signal vertex as a per-event systematic variation.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t14
title: "Summary plot 1SFH e Dirac (postfit)" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed yields in the different analysis regions (postfit) for the 1SFH e Dirac model (10 GeV, 10mm).
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.
DOI: 10.17182/hepdata.115511.v1/t8
title: "CL for 2QDH IH Majorana model" of "Search for heavy neutral leptons in decays of $W$ bosons using a dilepton displaced vertex in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Expected and observed 95% CL for the 2QDH IH Majorana model.
description: A search for a long-lived, heavy neutral lepton ($N$) in 139/fb of $\sqrt{s} = 13$ TeV $pp$ collision data collected by the ATLAS detector at the Large Hadron Collider is reported. 
The $N$ is produced via $W \rightarrow N \mu$ or $W \rightarrow N e$ and decays into two charged leptons and a neutrino, forming a displaced vertex.
The $N$ mass is reconstructed and used for background estimation.
No signal is observed, and limits are set on the squared mixing parameters of the $N$ with the left-handed neutrino states for the $N$ mass range $3$ GeV $&lt; m_N &lt; 15$ GeV. 
For the first time, limits are given for both single-flavor and multiflavor mixing scenarios motivated by neutrino flavor oscillation results for both the normal and inverted neutrino-mass hierarchies.

The class used to compute the HNL mass for each event can be found in 'Resources' -&gt; 'Common Resources' -&gt; 'HNLMassCalculation.py'.