cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.25574/29142
title: Chandra X-ray Observatory ObsId 29142

description: AO-23 Calibration Observations of HZ43
DOI: 10.25574/29166
title: Chandra X-ray Observatory ObsId 29166

description: AO-24 Cross-Calibration Observations of 3C273
DOI: 10.25574/29179
title: Chandra X-ray Observatory ObsId 29179

description: Simultaneous Chandra and XRISM Spectroscopy of NGC 4151
DOI: 10.15468/dl.7vfm2t
title: Occurrence Download

description: A dataset containing 17 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is Yoldia limatula",
 "Country is Netherlands",
 "HasCoordinate is true"
 ]
}

 The dataset includes 17 records from 3 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0009254-251009101135966/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.25574/29232
title: Chandra X-ray Observatory ObsId 29232

description: Characterizing the Energetics and Dynamics of V750 Ara, a gamma Cas-type Star
DOI: 10.17182/hepdata.25225.v1/t2
title: "Table 2" of "Exclusive eta production in proton-proton reactions."

description: Differential cross section for incident kinetic energy 2.50 GeV, divided by the phase space as a function of the invariant mass of the ETA and the final state proton with the lower value of ABS(T). This is proportional to the square of the decay matrix element ABS(M)**2 of the P-ETA system.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t3
title: "Table 3" of "Exclusive eta production in proton-proton reactions."

description: Differential cross section for incident kinetic energy 2.85 GeV, divided by the phase space as a function of the invariant mass of the ETA and the final state proton with the lower value of ABS(T). This is proportional to the square of the decay matrix element ABS(M)**2 of the P-ETA system.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t4
title: "Table 4" of "Exclusive eta production in proton-proton reactions."

description: Measured differential cross section as a function of the c.m. momentum of the ETA meson.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t5
title: "Table 5" of "Exclusive eta production in proton-proton reactions."

description: Measured differential cross section as a function of the proton momentum in the final state PP rest frame.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t6
title: "Table 6" of "Exclusive eta production in proton-proton reactions."

description: Measured angular distribution of the ETA meson w.r.t. the beam direction.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t7
title: "Table 7" of "Exclusive eta production in proton-proton reactions."

description: Measured angular distribution of the final state PP system w.r.t. the beam direction.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25225.v1/t8
title: "Table 8" of "Exclusive eta production in proton-proton reactions."

description: Analysing power as a function of the angular of the ETA meson in the c.m. system.
description: SACLAY SATURNE-II accelerator. Measurement of the exclusive production of ETA mesons in polarized proton-proton interactions with beam kinetic energies of 2.15, 2.50 and 2.85 GeV. The ETA meson is observed by the decay to PI+ PI- PI0 and results are presented for momentum and angular differential cross sections and polarizations.
DOI: 10.17182/hepdata.25226.v1/t1
title: "Table 1" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.975.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t2
title: "Table 2" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.925.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t3
title: "Table 3" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.875.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t10
title: "Table 10" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TT) for COS(THETA*) = -0.925.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t4
title: "Table 4" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(T) + EPSILON*SIG(L) for COS(THETA*) = -0.825.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t5
title: "Table 5" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TL) for COS(THETA*) = -0.975.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t6
title: "Table 6" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TL) for COS(THETA*) = -0.925.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t7
title: "Table 7" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TL) for COS(THETA*) = -0.875.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t8
title: "Table 8" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TL) for COS(THETA*) = -0.825.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t9
title: "Table 9" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TT) for COS(THETA*) = -0.975.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t11
title: "Table 11" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TT) for COS(THETA*) = -0.875.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25226.v1/t12
title: "Table 12" of "Backward electroproduction of pi0 mesons on protons in the region of nucleon resonances at four momentum transfer squared Q**2 = 1.0-GeV**2."

description: Cross section SIG(TT) for COS(THETA*) = -0.825.
description: Jefferson Lab-CEBAF. Hall A Collaboration. Measurement of the cross sections for backward electroproduction of PI0 mesons on protons using a 4 GeV electron beam. The data are at a Q**2 of 1 GeV**2 and an azimuthal angle of 75 degrees which is the angle between the leptonic and hadronic planes. The data are presented as a function of W, the centre of mass energies of the GAMMA* P system and COS(THETA*) where THETA* is the polar angle of the PI0 in the pion-proton system. Cross sections are given for the combination of longitudinal and transverse components SIG(L) + EPSILON*SIG(T) and inteference components SIG(TU) and SIG(TT). Epsilon is the virtual photon polarization.
DOI: 10.17182/hepdata.25227.v1/t1
title: "Table 1" of "K- p ---&gt; pi0 pi0 Sigma0 at p(K)- = 514-MeV/c to 750-MeV/c and comparison with other pi0 pi0 production"

description: Total cross section measurement. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 SIGMA0 for kaon momenta from 514 to 750 MeV.
DOI: 10.17182/hepdata.25228.v1/t1
title: "Table 1" of "Reaction K- p --&gt; pi0 pi0 lambda from p(K-) = 514-MeV/c to 750-MeV/c."

description: Measured cross section. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 LAMBDA for incident kaon momenta from 514 to 750 MeV.. Numerical values supplied by S. Prakhov.
DOI: 10.17182/hepdata.25228.v1/t2
title: "Table 2" of "Reaction K- p --&gt; pi0 pi0 lambda from p(K-) = 514-MeV/c to 750-MeV/c."

description: Differential cross section for the di-pion system in the c.m. system for incident momenta 514 to 629 MeV.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 LAMBDA for incident kaon momenta from 514 to 750 MeV.. Numerical values supplied by S. Prakhov.
DOI: 10.17182/hepdata.25228.v1/t3
title: "Table 3" of "Reaction K- p --&gt; pi0 pi0 lambda from p(K-) = 514-MeV/c to 750-MeV/c."

description: Differential cross section for the di-pion system in the c.m. system for incident momenta 659 to 750 MeV.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 LAMBDA for incident kaon momenta from 514 to 750 MeV.. Numerical values supplied by S. Prakhov.
DOI: 10.17182/hepdata.25228.v1/t4
title: "Table 4" of "Reaction K- p --&gt; pi0 pi0 lambda from p(K-) = 514-MeV/c to 750-MeV/c."

description: Polarization of the LAMBDA as a function of the c.m. amgle of the 2 pion system for incident energies 514 to 629 MeV.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 LAMBDA for incident kaon momenta from 514 to 750 MeV.. Numerical values supplied by S. Prakhov.
DOI: 10.17182/hepdata.25228.v1/t5
title: "Table 5" of "Reaction K- p --&gt; pi0 pi0 lambda from p(K-) = 514-MeV/c to 750-MeV/c."

description: Polarization of the LAMBDA as a function of the c.m. amgle of the 2 pion system for incident energies 659 to 750 MeV.
description: BNL-AGS. Measurement of the cross section for the reaction K- P --& gt; PI0 PI0 LAMBDA for incident kaon momenta from 514 to 750 MeV.. Numerical values supplied by S. Prakhov.
DOI: 10.17182/hepdata.25230.v1/t1
title: "Table 1" of "Measurement of the pd ---&gt; pd eta cross section in complete kinematics"

description: Total cross section as a function of the incident proton kinetic energy and the excess energy Q given by SQRT(S)-M(P)-M(D)-M(ETA).
description: Svedberg Lab-Uppsala. Measurement of the cross section for the reaction P DEUT --& gt; P DEUT ETA at the CELSIUS storage ring. The data cover 5 proton kinetic energies from 0.927 to 1.096 GeV.
DOI: 10.17182/hepdata.25267.v1/t1
title: "Table 1" of "Elastic neutron scattering at 96 MeV from 12C and Pb-208"

description: Measured differential cross section for elastic scattering on PB208. The first DSYS systematic error is from the uncertainty in the contributions from multiple scattering corrections and the second DSYS refers to the cross section uncertainty due to the uncertainty in the angle measurement.
description: Svedberg Lab-Uppsala. Measurement of the cross section for elastic scattering on neutrons on Lead and Carbon nuclei at an incident neutron kinetic energy of 96 MeV.
DOI: 10.17182/hepdata.25267.v1/t2
title: "Table 2" of "Elastic neutron scattering at 96 MeV from 12C and Pb-208"

description: Measured differential cross section for elastic scattering on C12. The first DSYS systematic error is from the uncertainty in the contributions from multiple scattering corrections and the second DSYS refers to the cross section uncertainty due to the uncertainty in the angle measurement.
description: Svedberg Lab-Uppsala. Measurement of the cross section for elastic scattering on neutrons on Lead and Carbon nuclei at an incident neutron kinetic energy of 96 MeV.
DOI: 10.17182/hepdata.25268.v1/t1
title: "Table 1" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 139 GeV PI+ beam (standard track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.
DOI: 10.17182/hepdata.25268.v1/t2
title: "Table 2" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 139 GeV PI- beam (standard track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.
DOI: 10.17182/hepdata.25268.v1/t3
title: "Table 3" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 117 GeV PI- beam (standard track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.
DOI: 10.17182/hepdata.25268.v1/t4
title: "Table 4" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 98 GeV PI- beam (standard track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.
DOI: 10.17182/hepdata.25268.v1/t5
title: "Table 5" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 87 GeV PI- beam (standard track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.
DOI: 10.17182/hepdata.25268.v1/t6
title: "Table 6" of "Analyzing powers for pi p elastic scattering between 57 and 139 MeV"

description: Analysing power measurements for a 87 GeV PI- beam (short track).
description: TRIUMF. Measurement of the analysing powers in PI+- P polarised elastic scattering at incident energies from 57 to 139 MeV. The experiment uses the CHAOS spectrometer and a polarized spin target.. Standard track and short track refer to different trigger conditions. See text of article.