cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.25404.v1/t17
title: "Table 17" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 &lt; ET ARAP &lt; 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t18
title: "Table 18" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 &lt; ET ARAP &lt; 2.34, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t19
title: "Table 19" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 &lt; ET ARAP &lt; 2.18, is subdivided into eight nominally equal bins of 0.16 in pseud orapidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t20
title: "Table 20" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 &lt; ETA RAP &lt; 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudo rapidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t21
title: "Table 21" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 ETAR AP &lt; 2.50, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t22
title: "Table 22" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 ETAR AP &lt; 2.34, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t23
title: "Table 23" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 ETAR AP &lt; 2.18, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t24
title: "Table 24" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 ETARA P &lt; 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudora pidity.
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t25
title: "Table 25" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 ETAR AP &lt; 2.50, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t26
title: "Table 26" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 ETAR AP &lt; 2.34, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t27
title: "Table 27" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 ETAR AP &lt; 2.18, is subdivided into eight nominally equal bins of 0.16 in pseudor apidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25404.v1/t28
title: "Table 28" of "Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies"

description: ET is defined as the sum of Ei*Sin(THETAi) taken over all particles em itted on an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.7 ETARA P &lt; 2.02, is subdivided into eight nominally equal bins of 0.16 in pseudora pidity. ET distributions define centrality, tipically by a certain upper perc entile of the distribution. In the table centrality denoted as ZCAL(Zero de gree CALorimeter).
description: BNL-ION. Systematics of midrapidity transverse energy distributions in limited apertures from p+Be to Au+Au collisions at relativistic energies.
DOI: 10.17182/hepdata.25426.v1/t1
title: "Table 1" of "Fusion enhancement in the 32,38S+Ta-181 reaction"

description: A typical beam energy resolution was 0.01 TO 0.1 MeV. In the S32-induced reaction, an incomplete fussion component was observed at high energies, with an average linear momentum transfer corresponding to th e escape of an alpha patticle. The deduced interaction barrier heights were 130 .7+-0.3 and 124.8+-0.3 MeV for the S32 and S38-induced reactions respectively.
description: MSU-CYC and ANL-ATLAS. Fusion enhancement in the 32,38S+181Ta reaction.. S38 beam produced by projectile fragmentation (AR40 primary 40 MeV/nucleon beam and the production BE9 target).
DOI: 10.17182/hepdata.25426.v1/t2
title: "Table 2" of "Fusion enhancement in the 32,38S+Ta-181 reaction"

description: A typical beam energy resolution was 0.01 TO 0.1 MeV.
description: MSU-CYC and ANL-ATLAS. Fusion enhancement in the 32,38S+181Ta reaction.. S38 beam produced by projectile fragmentation (AR40 primary 40 MeV/nucleon beam and the production BE9 target).
DOI: 10.17182/hepdata.25427.v1/t1
title: "Table 1" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: Angular distribution for DEUT P elastic scattering at EKIN of 140 MeV with the SMART spectrograph.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t2
title: "Table 2" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: Angular distribution for DEUT P elastic scattering at EKIN of 270 MeV with the D-room polarimeter.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t3
title: "Table 3" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: Angular distribution for DEUT P elastic scattering at EKIN of 270 MeV with the SMART spectrograph.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t4
title: "Table 4" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: The vector and tensor analyzing powers in DEUT P elastic scattering at EKINof 140 MeV with the SMART spectrograph.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t5
title: "Table 5" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: The vector and tensor analyzing powers in DEUT P elastic scattering at EKINof 140 MeV with the D-room polarimeter.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t6
title: "Table 6" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: The vector and tensor analyzing powers in DEUT P elastic scattering at EKINof 200 MeV with the D-room polarimeter.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t7
title: "Table 7" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: The vector and tensor analyzing powers in DEUT P elastic scattering at EKINof 270 MeV with the SMART spectrograph.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25427.v1/t8
title: "Table 8" of "Complete set of precise deuteron analyzing powers at intermediate energies: Comparison with modern nuclear force predictions"

description: The vector and tensor analyzing powers in DEUT P elastic scattering at EKINof 270 MeV with the D-room polarimeter.
description: RIKEN accelerator. Measurement of the deuteron vector and tensor analyzing powers in deuteron proton elastic scattering at incident kinetic energies of 140, 200 and 270 MeV. Angular distributions are also given.
DOI: 10.17182/hepdata.25429.v1/t1
title: "Table 1" of "Loss of memory of target nucleus deformation axis in heavy ion fusion fission"

description: No description provided.
description: ANUC-CYC accelerator. The FUSION cross sections SIG(C=FUS) were obtained by summing SIG(C=ER) and SIG(C=FIS).
DOI: 10.17182/hepdata.25430.v1/t1
title: "Table 1" of "Reaction mechanisms and multifragmentation processes in Zn-64 + Ni-58 at 35A-MeV to 79A-MeV"

description: No description provided.
description: GANIL accelerator. GANIL E-160 Collaboration. Reaction mechanisms and multifragmentation processes in 64Zn+58Ni at 35A-79A MeV.
DOI: 10.17182/hepdata.25430.v1/t2
title: "Table 2" of "Reaction mechanisms and multifragmentation processes in Zn-64 + Ni-58 at 35A-MeV to 79A-MeV"

description: Average summed transverse momentum.
description: GANIL accelerator. GANIL E-160 Collaboration. Reaction mechanisms and multifragmentation processes in 64Zn+58Ni at 35A-79A MeV.
DOI: 10.17182/hepdata.25434.v1/t1
title: "Table 1" of "Alpha breakup of Li-6 and Li-7 near the Coulomb barrier"

description: No description provided.
description: VAN-DE-GRAAFF and LINAC. Florida State University Tandem Accelerator Laboratory. alpha breakup of 6Li and 7Li near the Coulomb barrier.
DOI: 10.17182/hepdata.25434.v1/t2
title: "Table 2" of "Alpha breakup of Li-6 and Li-7 near the Coulomb barrier"

description: No description provided.
description: VAN-DE-GRAAFF and LINAC. Florida State University Tandem Accelerator Laboratory. alpha breakup of 6Li and 7Li near the Coulomb barrier.
DOI: 10.17182/hepdata.25442.v1/t1
title: "Table 1" of "Charged particle production in the Pb + Pb system at 158-GeV/c per nucleon."

description: Q(NAME=B) parameter is the total sum of the individual charges of the projectile fragments.
description: Charged particle production in the Pb + Pb system at 158 GeV/c per nucleon. CERN-SPS accelerator. The previous data were published in PR C53, 3044.
DOI: 10.17182/hepdata.25444.v1/t1
title: "Table 1" of "Study of a $K^0_S K^0_S$ Plus Threshold Enhancement Observed in the Final States $\bar{p} p \to K^0_S K^0_S$ Pions at 700-{MeV}/$c$ to 760-{MeV}/$c$"

description: No description provided.
description: SACLAY 80-CM HBC. ANALYSIS OF KS KS SYSTEM NEAR THRESHOLD. RESONANCE PRODUCTION CROSS SECTIONS GIVEN HERE.
DOI: 10.17182/hepdata.25444.v1/t2
title: "Table 2" of "Study of a $K^0_S K^0_S$ Plus Threshold Enhancement Observed in the Final States $\bar{p} p \to K^0_S K^0_S$ Pions at 700-{MeV}/$c$ to 760-{MeV}/$c$"

description: FIT TO RESONANCE PRODUCTION CHANNELS IN FINAL STATE.
description: SACLAY 80-CM HBC. ANALYSIS OF KS KS SYSTEM NEAR THRESHOLD. RESONANCE PRODUCTION CROSS SECTIONS GIVEN HERE.
DOI: 10.17182/hepdata.25444.v1/t3
title: "Table 3" of "Study of a $K^0_S K^0_S$ Plus Threshold Enhancement Observed in the Final States $\bar{p} p \to K^0_S K^0_S$ Pions at 700-{MeV}/$c$ to 760-{MeV}/$c$"

description: FIT TO RESONANCE PRODUCTION CHANNELS IN FINAL STATE.
description: SACLAY 80-CM HBC. ANALYSIS OF KS KS SYSTEM NEAR THRESHOLD. RESONANCE PRODUCTION CROSS SECTIONS GIVEN HERE.
DOI: 10.17182/hepdata.25461.v1/t1
title: "Table 1" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t2
title: "Table 2" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t3
title: "Table 3" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t4
title: "Table 4" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t5
title: "Table 5" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t6
title: "Table 6" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t7
title: "Table 7" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t10
title: "Table 10" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t8
title: "Table 8" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t9
title: "Table 9" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t11
title: "Table 11" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t12
title: "Table 12" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t13
title: "Table 13" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.
DOI: 10.17182/hepdata.25461.v1/t14
title: "Table 14" of "Strong absorption radii from reaction cross-section measurements for neutron-rich nuclei"

description: No description provided.
description: MSU-CYC accelerator. The experimental detalies are similar to those used in earlier work (see PR C56, 250). The secondary radiative beams were produced through the projectile fragmentation of MN55 primery beam on BE9 target. The quoted errors were obtained by considering the statistical errors and those associated to the range evaluation.