cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.81727.v1/t4
title: "Table 4" of "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $-0.96 \lt y \lt 0.04$ as a function of $p_{\rm {T}}$.
description: The $p_{\rm {T}}$-differential production cross section of prompt $\Lambda_{\rm {c}}^{+}$ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV at midrapidity. The $\Lambda_{\rm {c}}^{+}$ and $\Lambda_{\rm {c}}^{-}$ were reconstructed in the hadronic decay modes $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{-}\pi^{+}$, $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{0}_{S}$ and in the semileptonic channel $\Lambda_{\rm {c}}^{+}\to e^{+} \nu_{e} \Lambda$ (and charge conjugates). The measured values of the $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio, which is sensitive to the c-quark hadronisation mechanism, and in particular to the production of baryons, are presented and are larger than those measured previously in different colliding systems, centre-of-mass energies, rapidity and $p_{\rm {T}}$ intervals, where the $\Lambda_{\rm {c}}^{+}$ production process may differ. The results are compared with the expectations obtained from perturbative Quantum Chromodynamics calculations and Monte Carlo event generators. Neither perturbative QCD calculations nor Monte Carlo models reproduce the data, indicating that the fragmentation of heavy-flavour baryons is not well understood. The first measurement at the LHC of the $\Lambda_{\rm {c}}^{+}$~nuclear modification factor, $R_\mathrm{pPb}$, is also presented. The $R_\mathrm{pPb}$ is found to be consistent with unity and with that of D mesons within the uncertainties, and consistent with a theoretical calculation that includes cold nuclear matter effects and a calculation that includes charm quark interactions with a deconfined medium.
DOI: 10.17182/hepdata.81727.v1/t5
title: "Table 5" of "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in pp collisions at $\sqrt{s} = 7$ TeV in the transverse momentum interval $ 1 \lt p_{\rm T} \lt 8$ GeV/c and in the rapidity interval $|y|&lt;0.5$.
description: The $p_{\rm {T}}$-differential production cross section of prompt $\Lambda_{\rm {c}}^{+}$ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV at midrapidity. The $\Lambda_{\rm {c}}^{+}$ and $\Lambda_{\rm {c}}^{-}$ were reconstructed in the hadronic decay modes $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{-}\pi^{+}$, $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{0}_{S}$ and in the semileptonic channel $\Lambda_{\rm {c}}^{+}\to e^{+} \nu_{e} \Lambda$ (and charge conjugates). The measured values of the $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio, which is sensitive to the c-quark hadronisation mechanism, and in particular to the production of baryons, are presented and are larger than those measured previously in different colliding systems, centre-of-mass energies, rapidity and $p_{\rm {T}}$ intervals, where the $\Lambda_{\rm {c}}^{+}$ production process may differ. The results are compared with the expectations obtained from perturbative Quantum Chromodynamics calculations and Monte Carlo event generators. Neither perturbative QCD calculations nor Monte Carlo models reproduce the data, indicating that the fragmentation of heavy-flavour baryons is not well understood. The first measurement at the LHC of the $\Lambda_{\rm {c}}^{+}$~nuclear modification factor, $R_\mathrm{pPb}$, is also presented. The $R_\mathrm{pPb}$ is found to be consistent with unity and with that of D mesons within the uncertainties, and consistent with a theoretical calculation that includes cold nuclear matter effects and a calculation that includes charm quark interactions with a deconfined medium.
DOI: 10.5281/zenodo.17515420
title: Supplemental Data "Memory B cell Development in Response to mRNA SARS-CoV-2 and Nanoparticle Immunization in Mice"

description: Support data for the manuscript "Memory B cell Development in Response to mRNA SARS-CoV-2 and Nanoparticle Immunization in Mice" in bioRxiv.
description: Table 1. Sequences of anti-SARS-CoV-2 RBD IgG antibodies. Sequences derived from each mouse are shown separately for homotypic beta, mosaic 8b, and mRNA. Clonally related sequences (same V and J genes for heavy and light chains and similar CDR3) share the same background color; white background indicates singlets. 

Table 2. Sequences of monoclonal IgG antibodies produced. The first column of the table is the name of the antibody produced, followed by the nucleotide sequence of the paired heavy chain in blue and light chain in white.
DOI: 10.17182/hepdata.81727.v1/t6
title: "Table 6" of "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio measured in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the transverse momentum interval $2 \lt p_{\rm T} \lt 12$ GeV/c and in the rapidity interval $-0.96 \lt y \lt 0.04$.
description: The $p_{\rm {T}}$-differential production cross section of prompt $\Lambda_{\rm {c}}^{+}$ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV at midrapidity. The $\Lambda_{\rm {c}}^{+}$ and $\Lambda_{\rm {c}}^{-}$ were reconstructed in the hadronic decay modes $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{-}\pi^{+}$, $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{0}_{S}$ and in the semileptonic channel $\Lambda_{\rm {c}}^{+}\to e^{+} \nu_{e} \Lambda$ (and charge conjugates). The measured values of the $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio, which is sensitive to the c-quark hadronisation mechanism, and in particular to the production of baryons, are presented and are larger than those measured previously in different colliding systems, centre-of-mass energies, rapidity and $p_{\rm {T}}$ intervals, where the $\Lambda_{\rm {c}}^{+}$ production process may differ. The results are compared with the expectations obtained from perturbative Quantum Chromodynamics calculations and Monte Carlo event generators. Neither perturbative QCD calculations nor Monte Carlo models reproduce the data, indicating that the fragmentation of heavy-flavour baryons is not well understood. The first measurement at the LHC of the $\Lambda_{\rm {c}}^{+}$~nuclear modification factor, $R_\mathrm{pPb}$, is also presented. The $R_\mathrm{pPb}$ is found to be consistent with unity and with that of D mesons within the uncertainties, and consistent with a theoretical calculation that includes cold nuclear matter effects and a calculation that includes charm quark interactions with a deconfined medium.
DOI: 10.17182/hepdata.81727.v1/t7
title: "Table 7" of "$\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: The nuclear modification factor $R_\mathrm{pPb}$ of prompt $\Lambda_{\rm {c}}^{+}$ baryons in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV in the rapidity interval $ -0.96\lt y \lt 0.04$.
description: The $p_{\rm {T}}$-differential production cross section of prompt $\Lambda_{\rm {c}}^{+}$ charmed baryons was measured with the ALICE detector at the Large Hadron Collider (LHC) in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm {NN}}} = 5.02$ TeV at midrapidity. The $\Lambda_{\rm {c}}^{+}$ and $\Lambda_{\rm {c}}^{-}$ were reconstructed in the hadronic decay modes $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{-}\pi^{+}$, $\Lambda_{\rm {c}}^{+} \to {\rm p} {\rm K}^{0}_{S}$ and in the semileptonic channel $\Lambda_{\rm {c}}^{+}\to e^{+} \nu_{e} \Lambda$ (and charge conjugates). The measured values of the $\Lambda_{\rm {c}}^{+}$/${\rm D}^{0}$ ratio, which is sensitive to the c-quark hadronisation mechanism, and in particular to the production of baryons, are presented and are larger than those measured previously in different colliding systems, centre-of-mass energies, rapidity and $p_{\rm {T}}$ intervals, where the $\Lambda_{\rm {c}}^{+}$ production process may differ. The results are compared with the expectations obtained from perturbative Quantum Chromodynamics calculations and Monte Carlo event generators. Neither perturbative QCD calculations nor Monte Carlo models reproduce the data, indicating that the fragmentation of heavy-flavour baryons is not well understood. The first measurement at the LHC of the $\Lambda_{\rm {c}}^{+}$~nuclear modification factor, $R_\mathrm{pPb}$, is also presented. The $R_\mathrm{pPb}$ is found to be consistent with unity and with that of D mesons within the uncertainties, and consistent with a theoretical calculation that includes cold nuclear matter effects and a calculation that includes charm quark interactions with a deconfined medium.
DOI: 10.17182/hepdata.81935.v1/t1
title: "Table 1" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The measured W+W+ EWK fiducual cross section.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t2
title: "Table 2" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Data and estimated signal and background yields after the selection in the two dimensional dijet-dilepton mass distributions. This is used for the standard model measurements.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t3
title: "Table 3" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Data and estimated signal and background yields after the selection in the one dimensional dilepton mass distribution. This is used for the evaluation of the anomalous coupling limits.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t4
title: "Table 5" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Expected and observed 95% CL upper limits on the cross section times branching fraction, $\sigma_{\mathrm{VBF}}(H^{\pm\pm}) \times \mathrm{{\it B}}(H^{\pm\pm} \to W^{\pm}W^{\pm})$, as a function of doubly charged Higgs boson mass.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t5
title: "Table 6" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Expected and observed 95% CL upper limits on $s_H$ in the Georgi--Machacek model as a function of doubly charged Higgs boson mass.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t6
title: "Table 4" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Observed and expected 95% CL limits on the coefficients for higher-order (dimension-eight) operators in the effective field theory Lagrangian.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t7
title: "Table 7" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Main systematic uncertainties in the analysis.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81935.v1/t8
title: "Table 8" of "Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: Signal efficiency from the generator level fiducial definition to the reconstruction level selection for the dilepton mass variable.
description: The first observation of electroweak production of same-sign W boson pairs in proton-proton collisions is reported. The data sample corresponds to an integrated luminosity of 35.9fb-1 collected at a center-of-mass energy of 13TeV with the CMS detector at the LHC. Events are selected by requiring exactly two leptons (electrons or muons) of the same charge, moderate missing transverse momentum, and two jets with a large rapidity separation and a large dijet mass. The observed significance of the signal is 5.5 standard deviations, where a significance of 5.7 standard deviations is expected based on the standard model. The ratio of measured event yields to that expected from the standard model at leading-order is 0.90 +/- 0.22. A cross section measurement in a fiducial region is reported. Bounds are given on the structure of quartic vector boson interactions in the framework of dimension-eight effective field theory operators and on the production of doubly charged Higgs bosons.
DOI: 10.17182/hepdata.81936.v1/t1
title: "Table 1" of "Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured and expected fiducial cross-sections.
description: A measurement of vector boson scattering and constraints on anomalous quartic gauge couplings from events with two Z bosons and two jets are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector and corresponding to an integrated luminosity of 35.9 fb−1. The measurement is performed in the decay channel where each Z boson decays to either a pair of electrons or a pair of muons. The fiducial region is defined as: ptLepton &gt; 5 GeV, |etaLepton|&lt; 2.5,pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7, pTj2 &gt; 30 GeV, |etaj2|&lt; 4.7, mjj &gt; 100 GeV.
DOI: 10.17182/hepdata.81936.v1/t2
title: "Table 2" of "Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: Observed and expected exclusion limits for the aQGC parameters at 95% CL, without any form factors.
description: A measurement of vector boson scattering and constraints on anomalous quartic gauge couplings from events with two Z bosons and two jets are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector and corresponding to an integrated luminosity of 35.9 fb−1. The measurement is performed in the decay channel where each Z boson decays to either a pair of electrons or a pair of muons. The fiducial region is defined as: ptLepton &gt; 5 GeV, |etaLepton|&lt; 2.5,pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7, pTj2 &gt; 30 GeV, |etaj2|&lt; 4.7, mjj &gt; 100 GeV.
DOI: 10.17182/hepdata.81936.v2/t1
title: "Table 1" of "Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: Measured and expected fiducial cross-sections.
description: CERN LHC. A measurement of vector boson scattering and constraints on anomalous quartic gauge couplings from events with two Z bosons and two jets are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector and corresponding to an integrated luminosity of 35.9 fb−1. The measurement is performed in the decay channel where each Z boson decays to either a pair of electrons or a pair of muons. The fiducial region is defined as: ptLepton &gt; 5 GeV, |etaLepton|&lt; 2.5,pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7, pTj2 &gt; 30 GeV, |etaj2|&lt; 4.7, mjj &gt; 100 GeV.
DOI: 10.17182/hepdata.81936.v2/t2
title: "Table 2" of "Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton-proton collisions at sqrt(s) = 13 TeV"

description: Data from Table 2. Observed and expected exclusion limits for the aQGC parameters at 95% CL, without any form factors.
description: CERN LHC. A measurement of vector boson scattering and constraints on anomalous quartic gauge couplings from events with two Z bosons and two jets are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector and corresponding to an integrated luminosity of 35.9 fb−1. The measurement is performed in the decay channel where each Z boson decays to either a pair of electrons or a pair of muons. The fiducial region is defined as: ptLepton &gt; 5 GeV, |etaLepton|&lt; 2.5,pTj1 &gt; 30 GeV, |etaj1| &lt; 4.7, pTj2 &gt; 30 GeV, |etaj2|&lt; 4.7, mjj &gt; 100 GeV.