cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64728.v1/t3
title: "Table 3" of "The differential production cross section of the phi(1020) meson in sqrt(s)=7 TeV pp collisions measured with the ATLAS detector"

description: The integrated PHI(1020) meson production cross section in the fiducial region.
description: CERN-LHC. A measurement is presented of the PHI --&gt; K+ K- production cross section at sqrt(s) = 7 TeV using pp collision data corresponding to an integrated luminosity of 383 mub^{-1}, collected with the ATLAS experiment at the LHC in April 2010. Selection of PHI(1020) mesons is based on the identification of charged kaons by their energy loss in the pixel detector. The differential cross section is measured as a function of the transverse momentum, PT(PHI), and rapidity, ABS(YRAP(PHI)), of the phi(1020) meson in the fiducial region 500 &lt; PT(PHI) &lt; 1200 MeV, ABS(YRAP(PHI)) &lt; 0.8, kaon transverse momentum PT(K) &gt; 230 MeV and kaon momentum P(K) &lt; 800 MeV.
DOI: 10.17182/hepdata.64729.v1/t1
title: "Table 1" of "Measurements of the t t-bar charge asymmetry using the dilepton decay channel in pp collisions at sqrt(s) = 7 TeV"

description: The unfolded ASYMC and ASYMC(LEPTON) measurements.
description: CERN-LHC. The t t-bar charge asymmetry in proton-proton collisions at sqrt(s) = 7 TeV is measured using the dilepton decay channel (E+ E-, E+- MU-+ or MU+ MU-). The data correspond to a total integrated luminosity of 5.0 inverse-femtobarns, collected by the CMS experiment at the LHC. The top-antitop and lepton charge asymmetries, ASYMC and ASYMC(LEPTON), defined as the differences in absolute values of the rapidities between the reconstructed top quarks and antiquarks and of the pseudorapidities between the positive and negative leptons, respectively, are presented. The lepton charge asymmetry is also measured as a function of the invariant mass, M(TOP TOPBAR), rapidity, YRAP(TOP TOPBAR), and transverse momentum, PT(TOP TOPBAR), of the top-antitop system.
DOI: 10.17182/hepdata.64729.v1/t2
title: "Table 2" of "Measurements of the t t-bar charge asymmetry using the dilepton decay channel in pp collisions at sqrt(s) = 7 TeV"

description: Measurements of the unfolded ASYMC(LEPTON) values in bins of M(TOP TOPBAR).
description: CERN-LHC. The t t-bar charge asymmetry in proton-proton collisions at sqrt(s) = 7 TeV is measured using the dilepton decay channel (E+ E-, E+- MU-+ or MU+ MU-). The data correspond to a total integrated luminosity of 5.0 inverse-femtobarns, collected by the CMS experiment at the LHC. The top-antitop and lepton charge asymmetries, ASYMC and ASYMC(LEPTON), defined as the differences in absolute values of the rapidities between the reconstructed top quarks and antiquarks and of the pseudorapidities between the positive and negative leptons, respectively, are presented. The lepton charge asymmetry is also measured as a function of the invariant mass, M(TOP TOPBAR), rapidity, YRAP(TOP TOPBAR), and transverse momentum, PT(TOP TOPBAR), of the top-antitop system.
DOI: 10.17182/hepdata.64729.v1/t3
title: "Table 3" of "Measurements of the t t-bar charge asymmetry using the dilepton decay channel in pp collisions at sqrt(s) = 7 TeV"

description: Measurements of the unfolded ASYMC(LEPTON) values in bins of ABS(YRAP(TOP TOPBAR)).
description: CERN-LHC. The t t-bar charge asymmetry in proton-proton collisions at sqrt(s) = 7 TeV is measured using the dilepton decay channel (E+ E-, E+- MU-+ or MU+ MU-). The data correspond to a total integrated luminosity of 5.0 inverse-femtobarns, collected by the CMS experiment at the LHC. The top-antitop and lepton charge asymmetries, ASYMC and ASYMC(LEPTON), defined as the differences in absolute values of the rapidities between the reconstructed top quarks and antiquarks and of the pseudorapidities between the positive and negative leptons, respectively, are presented. The lepton charge asymmetry is also measured as a function of the invariant mass, M(TOP TOPBAR), rapidity, YRAP(TOP TOPBAR), and transverse momentum, PT(TOP TOPBAR), of the top-antitop system.
DOI: 10.34943/ed90224e-fc80-4374-9752-13256376a479
title: Burrard Inlet Hydrophone Deployed 2024-02-06

description: The Ocean Sonics icListen HF Hydrophone 1354 was deployed on 2024-02-06 at Burrard Inlet. Burrard Inlet is a coastal fjord in southwestern British Columbia. This device is a Hydrophone. Hydrophones are devices containing transducers that convert underwater sound waves into electrical signals. They are acoustic instruments that can process data while they are being collected to produce calibrated waveform data. Hydrophones are typically used to study vocalizations of marine mammals, ship traffic and ambient noise. It was deployed on a fixed platform. Data from this deployment were archived and made available through Ocean Networks Canada's Oceans 3.0 digital infrastructure, with quality assurance and derived data products following established practices.
DOI: 10.17182/hepdata.64729.v1/t4
title: "Table 4" of "Measurements of the t t-bar charge asymmetry using the dilepton decay channel in pp collisions at sqrt(s) = 7 TeV"

description: Measurements of the unfolded ASYMC(LEPTON) values in bins of PT(TOP TOPBAR).
description: CERN-LHC. The t t-bar charge asymmetry in proton-proton collisions at sqrt(s) = 7 TeV is measured using the dilepton decay channel (E+ E-, E+- MU-+ or MU+ MU-). The data correspond to a total integrated luminosity of 5.0 inverse-femtobarns, collected by the CMS experiment at the LHC. The top-antitop and lepton charge asymmetries, ASYMC and ASYMC(LEPTON), defined as the differences in absolute values of the rapidities between the reconstructed top quarks and antiquarks and of the pseudorapidities between the positive and negative leptons, respectively, are presented. The lepton charge asymmetry is also measured as a function of the invariant mass, M(TOP TOPBAR), rapidity, YRAP(TOP TOPBAR), and transverse momentum, PT(TOP TOPBAR), of the top-antitop system.
DOI: 10.17182/hepdata.64737.v1/t1
title: "Table 1" of "Search for $s$-channel Single Top Quark Production in the Missing Energy Plus Jets Sample using the Full CDF II Data Set"

description: The s-channel single top quark cross section measured assuming top quarks of mass 172.5 GeV. The measurement uses a sample of events with large missing transverse energy, two or three jets of which one or more are b-tagged and no detected electron or muon candidates.
description: Fermilab-Tevatron. The first search for single top quark production from the exchange of an s-channel virtual W boson using events with an imbalance in the total transverse momentum, b-tagged jets, and no identified leptons is presented. The full data set collected by the Collider Detector at Fermilab in the period 2001-2011, corresponding to an integrated luminosity of 9.45 fb^{-1} from Fermilab Tevatron proton-antiproton collisions at a center of mass energy of 1.96 TeV, is used.
DOI: 10.17182/hepdata.64737.v1/t2
title: "Table 2" of "Search for $s$-channel Single Top Quark Production in the Missing Energy Plus Jets Sample using the Full CDF II Data Set"

description: The combined s-channel single top quark cross section measurement assuming top quarks of mass 172.5 GeV. The measurement uses two samples of events. The first sample includes events with large missing transverse energy, two or three jets of which one or more are b-tagged and no detected electron or muon candidates. The second sample includes events with large missing transverse energy, one isolated muon or electron and two jets, at least one of which is b-tagged.
description: Fermilab-Tevatron. The first search for single top quark production from the exchange of an s-channel virtual W boson using events with an imbalance in the total transverse momentum, b-tagged jets, and no identified leptons is presented. The full data set collected by the Collider Detector at Fermilab in the period 2001-2011, corresponding to an integrated luminosity of 9.45 fb^{-1} from Fermilab Tevatron proton-antiproton collisions at a center of mass energy of 1.96 TeV, is used.
DOI: 10.17182/hepdata.64738.v1/t1
title: "Table 1" of "Indirect measurement of $\sin^2 \theta_W$ (or $M_W$) using $\mu^+\mu^-$ pairs from $\gamma^*/Z$ bosons produced in $p\bar{p}$ collisions at a center-of-momentum energy of 1.96 TeV"

description: The measured value of SIN**2(THETAEFF(LEPTON)).
description: Fermilab-Tevatron. Drell-Yan lepton pairs are produced in the process PBAR P --&gt; MU+ MU- + X through an intermediate GAMMA*/Z boson. The forward-backward asymmetry in the polar-angle distribution of the MU- as a function of the invariant mass of the MU+ MU- pair is used to obtain the effective leptonic determination SIN**2(THETAEFF(LEPTON)) of the electroweak-mixing parameter SIN**2(THETA(W)), from which the value of SIN**2(THETA(W)) is derived assuming the standard model. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.2 fb^{-1} of integrated luminosity from PBAR P collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II (2001-2011) data set.
DOI: 10.17182/hepdata.64738.v1/t2
title: "Table 2" of "Indirect measurement of $\sin^2 \theta_W$ (or $M_W$) using $\mu^+\mu^-$ pairs from $\gamma^*/Z$ bosons produced in $p\bar{p}$ collisions at a center-of-momentum energy of 1.96 TeV"

description: The measured value of SIN**2(THETA(W)).
description: Fermilab-Tevatron. Drell-Yan lepton pairs are produced in the process PBAR P --&gt; MU+ MU- + X through an intermediate GAMMA*/Z boson. The forward-backward asymmetry in the polar-angle distribution of the MU- as a function of the invariant mass of the MU+ MU- pair is used to obtain the effective leptonic determination SIN**2(THETAEFF(LEPTON)) of the electroweak-mixing parameter SIN**2(THETA(W)), from which the value of SIN**2(THETA(W)) is derived assuming the standard model. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.2 fb^{-1} of integrated luminosity from PBAR P collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II (2001-2011) data set.
DOI: 10.17182/hepdata.64738.v1/t3
title: "Table 3" of "Indirect measurement of $\sin^2 \theta_W$ (or $M_W$) using $\mu^+\mu^-$ pairs from $\gamma^*/Z$ bosons produced in $p\bar{p}$ collisions at a center-of-momentum energy of 1.96 TeV"

description: The measured value of M(W).
description: Fermilab-Tevatron. Drell-Yan lepton pairs are produced in the process PBAR P --&gt; MU+ MU- + X through an intermediate GAMMA*/Z boson. The forward-backward asymmetry in the polar-angle distribution of the MU- as a function of the invariant mass of the MU+ MU- pair is used to obtain the effective leptonic determination SIN**2(THETAEFF(LEPTON)) of the electroweak-mixing parameter SIN**2(THETA(W)), from which the value of SIN**2(THETA(W)) is derived assuming the standard model. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.2 fb^{-1} of integrated luminosity from PBAR P collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II (2001-2011) data set.
DOI: 10.17182/hepdata.64738.v1/t4
title: "Table 4" of "Indirect measurement of $\sin^2 \theta_W$ (or $M_W$) using $\mu^+\mu^-$ pairs from $\gamma^*/Z$ bosons produced in $p\bar{p}$ collisions at a center-of-momentum energy of 1.96 TeV"

description: The fully corrected measurement of ASYM(FB) as a function of the muon-pair invariant mass.
description: Fermilab-Tevatron. Drell-Yan lepton pairs are produced in the process PBAR P --&gt; MU+ MU- + X through an intermediate GAMMA*/Z boson. The forward-backward asymmetry in the polar-angle distribution of the MU- as a function of the invariant mass of the MU+ MU- pair is used to obtain the effective leptonic determination SIN**2(THETAEFF(LEPTON)) of the electroweak-mixing parameter SIN**2(THETA(W)), from which the value of SIN**2(THETA(W)) is derived assuming the standard model. The measurement sample, recorded by the Collider Detector at Fermilab (CDF), corresponds to 9.2 fb^{-1} of integrated luminosity from PBAR P collisions at a center-of-momentum energy of 1.96 TeV, and is the full CDF Run II (2001-2011) data set.
DOI: 10.17182/hepdata.64745.v1/t1
title: "Table 1" of "Double parton interactions in photon + 3 jet and photon + b/c jet + 2 jet events in ppbar collisions at sqrt{s}=1.96 TeV"

description: The effective cross sections measured for the inclusive and heavy flavour event samples.
description: Fermilab-Tevatron. We determine the fraction of events with double parton (DP) scattering in a single ppbar collision at sqrt(s) = 1.96 TeV in samples of photon + 3 jet and photon + b/c jet + 2 jet events collected with the D0 detector after it was upgraded in 2006 and corresponding to an integrated luminosity of about 8.7 fb^{-1}. The photon + 3 jet and photon + b/c jet + 2 jet event samples are referred to as inclusive (INCL) and heavy flavour (HF) samples respectively. The effective cross sections, SIGEFF, are presented for both event samples using the same kinematic selections.
DOI: 10.17182/hepdata.64747.v1/t1
title: "Table 1" of "Evidence for $s$-Channel Single-Top-Quark Production in Events with one Charged Lepton and Two Jets at CDF"

description: The s-channel cross section, measured assuming a top-quark mass of 172.5 GeV. The charge conjugate reaction is also included in the analysis.
description: Fermilab-Tevatron. We report evidence for s-channel single-top-quark production in proton-antiproton collisions at center-of-mass energy sqrt(s) = 1.96 TeV using a data set that corresponds to an integrated luminosity of 9.4 fb^{-1} collected by the Collider Detector at Fermilab during 2001-2011. We select events consistent with the s-channel process including two jets and one leptonically decaying W boson.
DOI: 10.17182/hepdata.64748.v1/t1
title: "Table 1" of "Measurement of the Production Cross Sections for a Z Boson and One or More b Jets in pp Collisions at $\sqrt{s} = 7$ TeV"

description: The cross section at the particle level for the production of a Z boson with exactly one b-jet.
description: CERN-LHC. The production of a Z boson, decaying into two leptons and produced in association with one or more b-jets, is studied using proton-proton collisions delivered by the LHC at a centre-of-mass energy of 7 TeV. The data were recorded in 2011 with the CMS detector and correspond to an integrated luminosity of 5 inverse femtobarns. The Z(ll) + b-jets cross sections (where ll = mu mu or ee) are measured separately for a Z boson produced with exactly one b-jet, with at least two b-jets and at least one b-jet. In addition, a cross section ratio is extracted for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet.
DOI: 10.17182/hepdata.64748.v1/t2
title: "Table 2" of "Measurement of the Production Cross Sections for a Z Boson and One or More b Jets in pp Collisions at $\sqrt{s} = 7$ TeV"

description: The cross section at the particle level for the production of a Z boson with at least two b-jets.
description: CERN-LHC. The production of a Z boson, decaying into two leptons and produced in association with one or more b-jets, is studied using proton-proton collisions delivered by the LHC at a centre-of-mass energy of 7 TeV. The data were recorded in 2011 with the CMS detector and correspond to an integrated luminosity of 5 inverse femtobarns. The Z(ll) + b-jets cross sections (where ll = mu mu or ee) are measured separately for a Z boson produced with exactly one b-jet, with at least two b-jets and at least one b-jet. In addition, a cross section ratio is extracted for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet.
DOI: 10.34943/6823b749-4102-40e7-b9bb-1ec8aa400cfe
title: Burrard Inlet Hydrophone Deployed 2025-01-25

description: The Ocean Sonics icListen HF Hydrophone 1354 was deployed on 2025-01-25 at Burrard Inlet. Burrard Inlet is a coastal fjord in southwestern British Columbia. This device is a Hydrophone. Hydrophones are devices containing transducers that convert underwater sound waves into electrical signals. They are acoustic instruments that can process data while they are being collected to produce calibrated waveform data. Hydrophones are typically used to study vocalizations of marine mammals, ship traffic and ambient noise. It was deployed on a fixed platform. Data from this deployment were archived and made available through Ocean Networks Canada's Oceans 3.0 digital infrastructure, with quality assurance and derived data products following established practices.
DOI: 10.17182/hepdata.64748.v1/t3
title: "Table 3" of "Measurement of the Production Cross Sections for a Z Boson and One or More b Jets in pp Collisions at $\sqrt{s} = 7$ TeV"

description: The cross section at the particle level for the production of a Z boson with at least one b-jet.
description: CERN-LHC. The production of a Z boson, decaying into two leptons and produced in association with one or more b-jets, is studied using proton-proton collisions delivered by the LHC at a centre-of-mass energy of 7 TeV. The data were recorded in 2011 with the CMS detector and correspond to an integrated luminosity of 5 inverse femtobarns. The Z(ll) + b-jets cross sections (where ll = mu mu or ee) are measured separately for a Z boson produced with exactly one b-jet, with at least two b-jets and at least one b-jet. In addition, a cross section ratio is extracted for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet.
DOI: 10.17182/hepdata.64748.v1/t4
title: "Table 4" of "Measurement of the Production Cross Sections for a Z Boson and One or More b Jets in pp Collisions at $\sqrt{s} = 7$ TeV"

description: The cross section ratio for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet of any flavour.
description: CERN-LHC. The production of a Z boson, decaying into two leptons and produced in association with one or more b-jets, is studied using proton-proton collisions delivered by the LHC at a centre-of-mass energy of 7 TeV. The data were recorded in 2011 with the CMS detector and correspond to an integrated luminosity of 5 inverse femtobarns. The Z(ll) + b-jets cross sections (where ll = mu mu or ee) are measured separately for a Z boson produced with exactly one b-jet, with at least two b-jets and at least one b-jet. In addition, a cross section ratio is extracted for a Z boson produced with at least one b-jet, relative to a Z boson produced with at least one jet.
DOI: 10.17182/hepdata.64754.v2/t1
title: "Table 1" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t2
title: "Table 2" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.34943/f6639f10-6d43-4c14-bcd3-60fe86da2f66
title: Burrard Inlet Hydrophone Deployed 2025-01-25

description: The Ocean Sonics icListen HF Hydrophone 1354 was deployed on 2025-01-25 at Burrard Inlet. Burrard Inlet is a coastal fjord in southwestern British Columbia. This device is a Hydrophone. Hydrophones are devices containing transducers that convert underwater sound waves into electrical signals. They are acoustic instruments that can process data while they are being collected to produce calibrated waveform data. Hydrophones are typically used to study vocalizations of marine mammals, ship traffic and ambient noise. It was deployed on a fixed platform. Data from this deployment were archived and made available through Ocean Networks Canada's Oceans 3.0 digital infrastructure, with quality assurance and derived data products following established practices.
DOI: 10.17182/hepdata.64754.v2/t3
title: "Table 3" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(SIN(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of PT(HADRON). The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t4
title: "Table 4" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of XB. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.
DOI: 10.17182/hepdata.64754.v2/t5
title: "Table 5" of "Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons"

description: ASYMUU(COS(PHI(HADRON))) asymmetries for positive and negative hadrons as a function of Z. The errors are statistical and systematic.
description: CERN-NA. Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at 160 GeV and a Li6D target during 2004. The amplitudes of the three azimuthal modulations COS(PHI(HADRON)), COS(2*PHI(HADRON)) and SIN(PHI(HADRON)), ASYMUU(COS(PHI(HADRON))), ASYMUU(COS(2*PHI(HADRON))) and ASYMUU(SIN(PHI(HADRON))) respectively, were obtained by binning the data separately in each of the relevant kinematic variables XB, Z or PT(HADRON) and binning in a three-dimensional grid of these three variables.