cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.76995.v1/t36
title: "Table 36" of "Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at sqrt(s)=8 TeV"

description: Average number of jets as a function of HT for events with one or more jets.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 19.6 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, and the scalar sum of jet transverse momenta (HT) for different jet multiplicities. Distributions of the angular correlations between the jets and the muon are examined, as well as the average number of jets as a function of HT and as a function of angular variables. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.1, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.5, and only jets with pT &gt; 30 GeV, |eta| &lt; 2.4, and a separation of deltaR &gt; 0.5 from the muon are considered.
DOI: 10.17182/hepdata.76995.v1/t37
title: "Table 37" of "Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at sqrt(s)=8 TeV"

description: Average number of jets as a function of HT for events with two or more jets.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 19.6 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, and the scalar sum of jet transverse momenta (HT) for different jet multiplicities. Distributions of the angular correlations between the jets and the muon are examined, as well as the average number of jets as a function of HT and as a function of angular variables. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.1, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.5, and only jets with pT &gt; 30 GeV, |eta| &lt; 2.4, and a separation of deltaR &gt; 0.5 from the muon are considered.
DOI: 10.17182/hepdata.76995.v1/t38
title: "Table 38" of "Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at sqrt(s)=8 TeV"

description: Average number of jets as a function of the rapidity difference between the two highest pT jets for events with two or more jets.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 19.6 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, and the scalar sum of jet transverse momenta (HT) for different jet multiplicities. Distributions of the angular correlations between the jets and the muon are examined, as well as the average number of jets as a function of HT and as a function of angular variables. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.1, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.5, and only jets with pT &gt; 30 GeV, |eta| &lt; 2.4, and a separation of deltaR &gt; 0.5 from the muon are considered.
DOI: 10.17182/hepdata.76995.v1/t39
title: "Table 39" of "Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at sqrt(s)=8 TeV"

description: Average number of jets as a function of the rapidity difference between the most forward and the most backward jets for events with two or more jets.
description: CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 19.6 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, and the scalar sum of jet transverse momenta (HT) for different jet multiplicities. Distributions of the angular correlations between the jets and the muon are examined, as well as the average number of jets as a function of HT and as a function of angular variables. The cross sections are measured in the fiducial region defined by a muon with pT &gt; 25 GeV and pseudorapidity |eta| &lt; 2.1, and by a transverse mass between the muon and the missing transverse energy MT &gt; 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.5, and only jets with pT &gt; 30 GeV, |eta| &lt; 2.4, and a separation of deltaR &gt; 0.5 from the muon are considered.
DOI: 10.17182/hepdata.76996.v1/t1
title: "Table 1" of "Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector"

description: Summary of central values and total systematical uncertainties for the $A_{FB}$ values unfolded for mass bin migration and dilution effects in the CC electron channel, CF electron channel and muon channel.
description: The Observable is calculated as a function of the di-lepton invariant mass. The forward backward asymmetry has been calculated at detector level and then corrected with an unfolding technique. Two corrections are applied: detector resolution and QED radiative corrections (namely mass bin migration), dilution. The results are presented for the cases when only the mass bin migration correction has been applied and when both the mass bin migration and dilution corrections have been applied. A measurements of $A_{FB}$ at Dressed level is also shown. The forward-backward asymmetry has been calculated for three different final states: electron Central-Central (CC), electron Central-Forward (CF) and muons. CC electrons are required to have $p_{T}&gt;25$ GeV and $|\eta|&lt;2.4$, CF electrons are required to have $p_{T}&gt;25$ GeV, one electron with $|\eta|&lt;2.4$ and one electron with $2.5&lt;|\eta|&lt;4.9$. Muons are required to have $p_{T}&gt;20$ GeV and $|\eta|&lt;2.4$. The $A_{FB}$ has been calculated for di-lepton invariant-masses $66
DOI: 10.17182/hepdata.76996.v1/t2
title: "Table 2" of "Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector"

description: Summary of central values and total systematical uncertainties for the unfolded $A_{FB}$ values which takes into account mass bin migration only in CC electron channel for Born and Dressed leptons. Dressed leptons are constructed by adding 4-vectors of the bare lepton and all real photons coming from the boson/lepton decay within a $\Delta R&lt;$0.1.
description: The Observable is calculated as a function of the di-lepton invariant mass. The forward backward asymmetry has been calculated at detector level and then corrected with an unfolding technique. Two corrections are applied: detector resolution and QED radiative corrections (namely mass bin migration), dilution. The results are presented for the cases when only the mass bin migration correction has been applied and when both the mass bin migration and dilution corrections have been applied. A measurements of $A_{FB}$ at Dressed level is also shown. The forward-backward asymmetry has been calculated for three different final states: electron Central-Central (CC), electron Central-Forward (CF) and muons. CC electrons are required to have $p_{T}&gt;25$ GeV and $|\eta|&lt;2.4$, CF electrons are required to have $p_{T}&gt;25$ GeV, one electron with $|\eta|&lt;2.4$ and one electron with $2.5&lt;|\eta|&lt;4.9$. Muons are required to have $p_{T}&gt;20$ GeV and $|\eta|&lt;2.4$. The $A_{FB}$ has been calculated for di-lepton invariant-masses $66
DOI: 10.17182/hepdata.76996.v1/t3
title: "Table 3" of "Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector"

description: Summary of central values and total systematical uncertainties for the unfolded $A_{FB}$ values which takes into account mass bin migration only in CF electron channel for Born and Dressed leptons. Dressed leptons are constructed by adding 4-vectors of the bare lepton and all real photons coming from the boson/lepton decay within a $\Delta R&lt;$0.1.
description: The Observable is calculated as a function of the di-lepton invariant mass. The forward backward asymmetry has been calculated at detector level and then corrected with an unfolding technique. Two corrections are applied: detector resolution and QED radiative corrections (namely mass bin migration), dilution. The results are presented for the cases when only the mass bin migration correction has been applied and when both the mass bin migration and dilution corrections have been applied. A measurements of $A_{FB}$ at Dressed level is also shown. The forward-backward asymmetry has been calculated for three different final states: electron Central-Central (CC), electron Central-Forward (CF) and muons. CC electrons are required to have $p_{T}&gt;25$ GeV and $|\eta|&lt;2.4$, CF electrons are required to have $p_{T}&gt;25$ GeV, one electron with $|\eta|&lt;2.4$ and one electron with $2.5&lt;|\eta|&lt;4.9$. Muons are required to have $p_{T}&gt;20$ GeV and $|\eta|&lt;2.4$. The $A_{FB}$ has been calculated for di-lepton invariant-masses $66
DOI: 10.17182/hepdata.76996.v1/t4
title: "Table 4" of "Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector"

description: Central values and total systematical uncertainties for the unfolded $A_{FB}$ values which takes into account mass bin migration only in muon channel for Born and Dressed leptons. Dressed leptons are constructed by adding 4-vectors of the bare lepton and all real photons coming from the boson/lepton decay within a $\Delta R&lt;$0.1.
description: The Observable is calculated as a function of the di-lepton invariant mass. The forward backward asymmetry has been calculated at detector level and then corrected with an unfolding technique. Two corrections are applied: detector resolution and QED radiative corrections (namely mass bin migration), dilution. The results are presented for the cases when only the mass bin migration correction has been applied and when both the mass bin migration and dilution corrections have been applied. A measurements of $A_{FB}$ at Dressed level is also shown. The forward-backward asymmetry has been calculated for three different final states: electron Central-Central (CC), electron Central-Forward (CF) and muons. CC electrons are required to have $p_{T}&gt;25$ GeV and $|\eta|&lt;2.4$, CF electrons are required to have $p_{T}&gt;25$ GeV, one electron with $|\eta|&lt;2.4$ and one electron with $2.5&lt;|\eta|&lt;4.9$. Muons are required to have $p_{T}&gt;20$ GeV and $|\eta|&lt;2.4$. The $A_{FB}$ has been calculated for di-lepton invariant-masses $66
DOI: 10.17182/hepdata.77001.v1/t1
title: "Table 1" of "Measurement of the $\pi^0$ electromagnetic transition form factor slope"

description: Number of reconstructed data events and MC events as a function of the Dalitz kinematic variable $x=(M_{ee}/M_{\pi^0})^2$. The MC events are reweighted to correspond to a TFF slope a=0. The MC sample is not normalized to the size of the data. The values of $x$ quoted in the table are the barycenters of the 50 variable size bins.
description: Number of Data and MC events in 50 bins of x
DOI: 10.17182/hepdata.77003.v1/t1
title: "Table 1" of "Search for two Higgs bosons in final states containing two photons and two bottom quarks"

description: Observed $m_\mathrm{jj}$ spectrum (black points) compared with a background estimate (black line), obtained in background only hypothesis, for HPHP category. The simulated radion resonances of $m_\mathrm{X} = 1.5$ and 2 TeV are also shown.
Observed and expected 95% CL upper limits on the product of cross section and the branching fraction sigma(pp-&gt;X)*B(X-&gt;HH) obtained through a combination of the two event categories. The limits for mX = 400 GeV are shown for both Low mass and High mass signal extraction methods.
description: CERN-LHC. A search is presented for the production of two Higgs bosons in final states containing two photons and two bottom quarks. Both resonant and nonresonant hypotheses are investigated. The analyzed data correspond to an integrated luminosity of 19.7 inverse femtobarns of proton-proton collisions at sqrt(s) = 8 TeV collected with the CMS detector. Good agreement is observed between data and predictions of the standard model (SM). Upper limits are set at 95% confidence level on the production cross section of new particles and compared to the prediction for the existence of a warped extra dimension. When the decay to two Higgs bosons is kinematically allowed, assuming a mass scale Lambda[R] = 1 TeV for the model, the data exclude a radion scalar at masses below 980 GeV. The first Kaluza-Klein excitation mode of the graviton in the RS1 Randall-Sundrum model is excluded for masses between 325 and 450 GeV. An upper limit of 0.71 pb is set on the nonresonant two-Higgs-boson cross section in the SM-like hypothesis. Limits are also derived on nonresonant production assuming anomalous Higgs boson couplings.
DOI: 10.17182/hepdata.77003.v1/t2
title: "Table 2" of "Search for two Higgs bosons in final states containing two photons and two bottom quarks"

description: Observed and expected 95% CL upper limits on the product of cross section and
the branching fraction sigma(pp-&gt;X)*B(X-&gt;HH-&gt;gamma gamma b b ) for the nonresonant BSM analysis, performed by changing the parameters 
$kappa_$lambda, y_t and c_2 while keeping all other parameters fixed at the SM predictions.
description: CERN-LHC. A search is presented for the production of two Higgs bosons in final states containing two photons and two bottom quarks. Both resonant and nonresonant hypotheses are investigated. The analyzed data correspond to an integrated luminosity of 19.7 inverse femtobarns of proton-proton collisions at sqrt(s) = 8 TeV collected with the CMS detector. Good agreement is observed between data and predictions of the standard model (SM). Upper limits are set at 95% confidence level on the production cross section of new particles and compared to the prediction for the existence of a warped extra dimension. When the decay to two Higgs bosons is kinematically allowed, assuming a mass scale Lambda[R] = 1 TeV for the model, the data exclude a radion scalar at masses below 980 GeV. The first Kaluza-Klein excitation mode of the graviton in the RS1 Randall-Sundrum model is excluded for masses between 325 and 450 GeV. An upper limit of 0.71 pb is set on the nonresonant two-Higgs-boson cross section in the SM-like hypothesis. Limits are also derived on nonresonant production assuming anomalous Higgs boson couplings.
DOI: 10.17182/hepdata.77003.v1/t3
title: "Table 3" of "Search for two Higgs bosons in final states containing two photons and two bottom quarks"

description: Signal efficiencies in the four different signal regions for the nonresonant BSM analysis, performed by changing the parameters 
$kappa_$lambda, y_t and c_2 while keeping all other parameters fixed at the SM predictions. 
The four signal regions are made in b-tag and m_HH categries, being those: "Low-purity, High-mass" (LPHM), "Low-purity, Low-mass" (LPLM), "High-purity, High-mass" (HPHM) and "High-purity, Low-mass" (HPLM).
description: CERN-LHC. A search is presented for the production of two Higgs bosons in final states containing two photons and two bottom quarks. Both resonant and nonresonant hypotheses are investigated. The analyzed data correspond to an integrated luminosity of 19.7 inverse femtobarns of proton-proton collisions at sqrt(s) = 8 TeV collected with the CMS detector. Good agreement is observed between data and predictions of the standard model (SM). Upper limits are set at 95% confidence level on the production cross section of new particles and compared to the prediction for the existence of a warped extra dimension. When the decay to two Higgs bosons is kinematically allowed, assuming a mass scale Lambda[R] = 1 TeV for the model, the data exclude a radion scalar at masses below 980 GeV. The first Kaluza-Klein excitation mode of the graviton in the RS1 Randall-Sundrum model is excluded for masses between 325 and 450 GeV. An upper limit of 0.71 pb is set on the nonresonant two-Higgs-boson cross section in the SM-like hypothesis. Limits are also derived on nonresonant production assuming anomalous Higgs boson couplings.
DOI: 10.17182/hepdata.77008.v1/t1
title: "Table 5" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The measured normalized $t\bar{t}$ double-differential cross sections in different bins of $y(t)$ and $p_{T}(t)$, along with their relative statistical and systematic uncertainties expressed as percentages.
description: No data abstract available.
DOI: 10.5517/ccdc.csd.cc2p5yhb
title: CSD 2478372: Experimental Crystal Structure Determination

description: Related Article: Yun-Hee Lee, Jin Kyun Kim, Yong-Jae Kim, Minju Kim, Yong Chan Cho, Rachel J. Husband, Cornelius Strohm, Emma Ehrenreich-Petersen, Konstantin Glazyrin, Torsten Laurus, Heinz Graafsma, Robert P. C. Bauer, Felix Lehmkühler, Karen Appel, Zuzana Konôpková, Minxue Tang, Anand Prashant Dwivedi, Jolanta Sztuck-Dambietz, Lisa Randolph, Khachiwan Buakor, Oliver Humphries, Carsten Baehtz, Tobias Eklund, Lisa Katharina Mohrbach, Anshuman Mondal, Hauke Marquardt, Earl Francis O’Bannon, Katrin Amann-Winkel, Choong-Shik Yoo, Ulf Zastrau, Hanns-Peter Liermann, Hiroki Nada, Geun Woo Lee|2025|Nat.Mater|||doi:10.1038/s41563-025-02364-x
description: An entry from the Inorganic Crystal Structure Database, the world’s repository for inorganic crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the joint CCDC and FIZ Karlsruhe Access Structures service and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.17182/hepdata.77008.v1/t2
title: "Table 6" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The correlation matrix of statistical uncertainties for the normalized $t\bar{t}$ double-differential cross sections as a function of $y(t)$ and $p_{T}(t)$. The values are expressed as percentages. For bin indices see Table 5.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t3
title: "Table 7" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: Sources and values of the relative systematic uncertainties in percent of the measured normalized $t\bar{t}$ double-differential cross sections as a function of $y(t)$ and $p_{T}(t)$. For bin indices see Table 5.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t4
title: "Table 8" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The measured normalized $t\bar{t}$ double-differential cross sections in different bins of $M(t\bar{t})$ and $y(t)$, along with their relative statistical and systematic uncertainties expressed as percentages.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t5
title: "Table 9" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The correlation matrix of statistical uncertainties for the normalized $t\bar{t}$ double-differential cross sections as a function of $M(t\bar{t})$ and $y(t)$. The values are expressed as percentages. For bin indices see Table 8.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t6
title: "Table 10" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: Sources and values of the relative systematic uncertainties in percent of the measured normalized $t\bar{t}$ double-differential cross sections as a function of $M(t\bar{t})$ and $y(t)$. For bin indices see Table 8.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t9
title: "Table 13" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: Sources and values of the relative systematic uncertainties in percent of the measured normalized $t\bar{t}$ double-differential cross sections as a function of $M(t\bar{t})$ and $y(t\bar{t})$. For bin indices see Table 11.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t10
title: "Table 14" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The measured normalized $t\bar{t}$ double-differential cross sections in different bins of $M(t\bar{t})$ and $\Delta \eta(t, \bar{t})$, along with their relative statistical and systematic uncertainties expressed as percentages.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t11
title: "Table 15" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: The correlation matrix of statistical uncertainties for the normalized $t\bar{t}$ double-differential cross sections as a function of $M(t\bar{t})$ and $\Delta \eta(t, \bar{t})$. The values are expressed as percentages. For bin indices see Table 14.
description: No data abstract available.
DOI: 10.17182/hepdata.77008.v1/t12
title: "Table 16" of "Measurement of double-differential cross sections for top quark pair production in pp collisions at sqrt(s) = 8 TeV and impact on parton distribution functions"

description: Sources and values of the relative systematic uncertainties in percent of the measured normalized $t\bar{t}$ double-differential cross sections as a function of $M(t\bar{t})$ and $\Delta \eta(t, \bar{t})$. For bin indices see Table 14.
description: No data abstract available.