cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64697.v1/t3
title: "Table 3" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The measured cross section and visible cross section for the three-body transition E+ E- --&gt; UPSILON(3S) PI+ PI-.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t4
title: "Table 4" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The product SIG( Zb+-(10610) PI-+ ) * BR( UPSILON(NS) PI-+ ) for N = 1, 2, 3.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t5
title: "Table 5" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The product SIG( Zb+-(10650) PI-+ ) * BR( UPSILON(NS) PI-+ ) for N = 1, 2, 3.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t6
title: "Table 6" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The Zb+-(10610) mass measured in each decay channel.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t7
title: "Table 7" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The Zb+-(10610) width measured in each decay channel.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t8
title: "Table 8" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The Zb+-(10650) mass measured in each decay channel.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64697.v1/t9
title: "Table 9" of "Amplitude analysis of e+e- =&gt; Y(nS)pi+pi- at sqrt(s)=10.865 GeV"

description: The Zb+-(10650) width measured in each decay channel.
description: KEK-BF. We report results on studies of the E+ E- annihilation into three-body UPSILON(NS) PI+ PI- (N=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The results are obtained with a 121.4 inverse femtobarn data sample collected with the Belle detector at the KEKB asymmetric-energy e+ e- collider. Amplitude analysis of the three-body UPSILON(NS) PI+ PI- final states strongly favors I(G) (J(P)) = 1+ (1+) quantum-number assignments for the two bottomonium-like Zb+- states, recently observed in the UPSILON(NS) PI+- and hb(MP) PI+- (m=1,2) decay channels.
DOI: 10.17182/hepdata.64698.v1/t1
title: "Table 1" of "Measurement of the Lepton Forward-Backward Asymmetry in Inclusive $B \rightarrow X_s \ell^+ \ell^-$ Decays"

description: The value of ASYM(FB) obtained from the fit in each of the four Q**2 bins.
description: KEK-BF. We report the first measurement of the lepton forward-backward asymmetry ASYM(FB) for the inclusive electroweak penguin process B --&gt; X(STRANGE) LEPTON+ LEPTON- as a function of Q**2 = M(LEPTON+ LEPTON-)**2, where LEPTON is an electron or a muon and X(STRANGE) is a hadronic recoil system with a strange quark. The results are based on a data sample containing 772*10**6 B BBAR pairs recorded at the UPSILON(4S) resonance, sqrt(s) = 10.56 GeV, with the Belle detector at the KEKB e+ e- collider. For Q**2 &gt; 10.2 GeV**2, ASYM(FB) &lt; 0 is excluded at the 2.3 SIGMA level, where SIGMA is the standard deviation. For Q**2 &lt; 4.3 GeV**2, the result is within 1.8 SIGMA of the theoretical expectation.
DOI: 10.17182/hepdata.64709.v1/t1
title: "Table 1" of "Invariant-Mass Distribution of Jet Pairs Produced in Association with a $W$ Boson in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV Using the Full CDF Run II Data Set"

description: The extracted cross section assuming that the new contribution (the excess over the expected background) has the same acceptance as that for a 140 GeV Higgs boson produced in association with a W boson.
description: Fermilab-Tevatron. We report on a study of the dijet invariant-mass distribution in events with one identified lepton, a significant imbalance in the total event transverse momentum, and two jets. This distribution is sensitive to the possible production of a new particle in association with a W boson, where the boson decays leptonically. We use the full data set of proton-antiproton collisions at 1.96 TeV center-of-mass energy collected by the Collider Detector at the Fermilab Tevatron during Run II (2001-2011) and corresponding to an integrated luminosity of 8.9 fb^{-1}. The data are found to be consistent with standard-model expectations, and a 95% confidence level upper limit of 0.9 pb is set on the cross section times branching ratio for production and decay into dijets of a new particle with mass of 144 GeV in association with a W boson.
DOI: 10.17182/hepdata.64709.v1/t2
title: "Table 2" of "Invariant-Mass Distribution of Jet Pairs Produced in Association with a $W$ Boson in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV Using the Full CDF Run II Data Set"

description: The extracted cross section measured with a restriction on DELTAR(JET1 JET2) and assuming that the new contribution (the excess over the expected background) has the same acceptance as that for a 140 GeV Higgs boson produced in association with a W boson.
description: Fermilab-Tevatron. We report on a study of the dijet invariant-mass distribution in events with one identified lepton, a significant imbalance in the total event transverse momentum, and two jets. This distribution is sensitive to the possible production of a new particle in association with a W boson, where the boson decays leptonically. We use the full data set of proton-antiproton collisions at 1.96 TeV center-of-mass energy collected by the Collider Detector at the Fermilab Tevatron during Run II (2001-2011) and corresponding to an integrated luminosity of 8.9 fb^{-1}. The data are found to be consistent with standard-model expectations, and a 95% confidence level upper limit of 0.9 pb is set on the cross section times branching ratio for production and decay into dijets of a new particle with mass of 144 GeV in association with a W boson.
DOI: 10.17182/hepdata.64710.v1/t1
title: "Table 1" of "Study of Top-Quark Production and Decays involving a Tau Lepton at CDF and Limits on a Charged-Higgs Boson Contribution"

description: The top-antitop quark production cross section measured assuming standard-model top-quark decays, TOP --&gt; W BOTTOM.
description: Fermilab-Tevatron. We present an analysis of top-antitop quark production and decay into a tau lepton, tau neutrino, and bottom quark. We use the full data set of proton-antiproton collisions at 1.96 TeV center-of-mass energy collected by the Collider Detector at the Fermilab Tevatron during Run II (2001-2011) and corresponding to an integrated luminosity of 9 fb^{-1}. Dilepton events where one lepton is an energetic electron or muon and the other a hadronically-decaying tau lepton are used. The branching fraction of top-quark decays into a charged Higgs boson and a bottom quark, which would imply violation of lepton universality, is limited to be less than 5.9% at 95% confidence level.
DOI: 10.17182/hepdata.64710.v1/t2
title: "Table 2" of "Study of Top-Quark Production and Decays involving a Tau Lepton at CDF and Limits on a Charged-Higgs Boson Contribution"

description: The branching fraction of the top quark into a tau lepton, a tau neutrino and a bottom quark.
description: Fermilab-Tevatron. We present an analysis of top-antitop quark production and decay into a tau lepton, tau neutrino, and bottom quark. We use the full data set of proton-antiproton collisions at 1.96 TeV center-of-mass energy collected by the Collider Detector at the Fermilab Tevatron during Run II (2001-2011) and corresponding to an integrated luminosity of 9 fb^{-1}. Dilepton events where one lepton is an energetic electron or muon and the other a hadronically-decaying tau lepton are used. The branching fraction of top-quark decays into a charged Higgs boson and a bottom quark, which would imply violation of lepton universality, is limited to be less than 5.9% at 95% confidence level.
DOI: 10.17182/hepdata.64710.v1/t3
title: "Table 3" of "Study of Top-Quark Production and Decays involving a Tau Lepton at CDF and Limits on a Charged-Higgs Boson Contribution"

description: The ratio of leptonic top branching ratios, 2 * BR(TOP --&gt; TAU NUTAU BOTTOM) / ( BR(TOP --&gt; E NUE BOTTOM) + BR(TOP --&gt; MU NUMU BOTTOM) ).
description: Fermilab-Tevatron. We present an analysis of top-antitop quark production and decay into a tau lepton, tau neutrino, and bottom quark. We use the full data set of proton-antiproton collisions at 1.96 TeV center-of-mass energy collected by the Collider Detector at the Fermilab Tevatron during Run II (2001-2011) and corresponding to an integrated luminosity of 9 fb^{-1}. Dilepton events where one lepton is an energetic electron or muon and the other a hadronically-decaying tau lepton are used. The branching fraction of top-quark decays into a charged Higgs boson and a bottom quark, which would imply violation of lepton universality, is limited to be less than 5.9% at 95% confidence level.
DOI: 10.17182/hepdata.64716.v1/t1
title: "Table 1" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: PI0 ASYM(LL) measurements from 2005.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t2
title: "Table 2" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: PI0 ASYM(LL) measurements from 2006.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t3
title: "Table 3" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: PI0 ASYM(LL) measurements from 2009.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t4
title: "Table 4" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: ETA ASYM(LL) measurements from 2005.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t5
title: "Table 5" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: ETA ASYM(LL) measurements from 2006.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t6
title: "Table 6" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: ETA ASYM(LL) measurements from 2009.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t7
title: "Table 7" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: Combined PI0 ASYM(LL) values from the PHENIX data sets at sqrt(s) = 200 GeV.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.34943/9135aa84-55d9-4a00-ae5f-a8fce45dcbec
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.64716.v1/t8
title: "Table 8" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: Combined ETA ASYM(LL) values from the PHENIX data sets at sqrt(s) = 200 GeV.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64716.v1/t9
title: "Table 9" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

description: The best fit value of the gluon polarization where the uncertainty is that at a chi-squared value of 9 when considering only statistical experimental uncertainties.
description: BNL-RHIC. Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, ASYM(LL), for PI0 and ETA production in sqrt(s) = 200 GeV polarized pp collisions. Comparison of the PI0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, DELTA(G), in the proton in the probed Bjorken x, XB, range. The effect of adding the new 2009 PI0 data to a recent global analysis of polarized scattering data is given.
DOI: 10.17182/hepdata.64717.v1/t1
title: "Table 1" of "Observation of s-Channel Production of Single Top Quarks at the Tevatron"

description: The measured cross section of single-top-quark production in the s channel.
description: Fermilab-Tevatron. We report the first observation of single-top-quark production in the s channel through the combination of the CDF and D0 measurements of the cross section in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV. The data sets correspond to total integrated luminosities of up to 9.7 fb^{-1} per experiment and were collected during Run II (2001-2011) of the Tevatron collider.
DOI: 10.17182/hepdata.64728.v1/t1
title: "Table 1" 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 differential PHI(1020) meson production cross section measured in the fiducial region as a function of the PHI(1020) transverse momentum.
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.64728.v1/t2
title: "Table 2" 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 differential PHI(1020) meson production cross section measured in the fiducial region as a function of the PHI(1020) rapidity.
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.