cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.25355.v1/t1
title: "Table 1" of "Measurement of pi- p --&gt; pi0 pi0 n from threshold to p(pi-) 750-MeV/c."

description: Measured total cross section. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction PI- P --& gt; PI0 PI0 N for incident pion momenta from threshold to 750 MeV/C.. Numerical values from S. Prakhov.
DOI: 10.17182/hepdata.25355.v1/t2
title: "Table 2" of "Measurement of pi- p --&gt; pi0 pi0 n from threshold to p(pi-) 750-MeV/c."

description: Differential angular distributions of the 2PI0 system for the LH2 data at beam momenta 355 to 472 MeV/c. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction PI- P --& gt; PI0 PI0 N for incident pion momenta from threshold to 750 MeV/C.. Numerical values from S. Prakhov.
DOI: 10.17182/hepdata.25355.v1/t3
title: "Table 3" of "Measurement of pi- p --&gt; pi0 pi0 n from threshold to p(pi-) 750-MeV/c."

description: Differential angular distributions of the 2PI0 system for the LH2 data at beam momenta 550 to 678 MeV/c. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction PI- P --& gt; PI0 PI0 N for incident pion momenta from threshold to 750 MeV/C.. Numerical values from S. Prakhov.
DOI: 10.17182/hepdata.25355.v1/t4
title: "Table 4" of "Measurement of pi- p --&gt; pi0 pi0 n from threshold to p(pi-) 750-MeV/c."

description: Differential angular distributions of the 2PI0 system for the LH2 data at beam momenta 691 to 727 MeV/c. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction PI- P --& gt; PI0 PI0 N for incident pion momenta from threshold to 750 MeV/C.. Numerical values from S. Prakhov.
DOI: 10.17182/hepdata.25355.v1/t5
title: "Table 5" of "Measurement of pi- p --&gt; pi0 pi0 n from threshold to p(pi-) 750-MeV/c."

description: Differential angular distributions of the 2PI0 system for the LH2 data at beam momenta 733 to 748 MeV/c. Statistical errors only.
description: BNL-AGS. Measurement of the cross section for the reaction PI- P --& gt; PI0 PI0 N for incident pion momenta from threshold to 750 MeV/C.. Numerical values from S. Prakhov.
DOI: 10.17182/hepdata.25392.v1/t1
title: "Table 1" of "Inclusive proton production cross-sections in (d, x p) reactions induced by 100-MeV deuterons"

description: All Cross Sections has errors 10 pct (for PB208 and U238 errors &gt;10 pct) including systematic uncertainties. Tabulated proton multiplicities extracted from the experimental data by dividing proton cross section by reaction cross section using the empirical expression pi*(1.58A**(1/3)+.671*Ad**(1/3))**2 (taken from PR B348, 697).
description: SAAC-CYC accelerator. A detailed layout of the facility can be found in PR C40, 1937. Inclusive proton production cross sections in (d,xp) reactions induced by 100 MeV deuterons.
DOI: 10.17182/hepdata.25393.v1/t1
title: "Table 1" of "Intermediate mass fragment emission in heavy ion collisions: Energy and system mass dependence"

description: Uncertainty in EKIN is 1 PCT.
description: MSU-CYC. Intermediate mass fragment emission in heavy-ion collisions: Energy and system mass dependence.. The targets were mounted at the center of MSU 4pi-Array detector system (see NIM A238, 347). To define the available energy in the center of mass of the system during the collision as accurately as possible, central collision events were chosen to be the 10% of all events for given beam-target combination which had the largest transverse energy.
DOI: 10.17182/hepdata.25394.v1/t1
title: "Table 1" of "Measurement of the n-p elastic scattering angular distribution at En=10 MeV"

description: Measured values of the N-P elastic scattering angular distributions. Data are normalized to the Breit-Hopkins total elastic cross section after radiative capture correction.
description: Ohio University Accelerator. Measurement of the N-P elastic scattering angular distribution at incident neutron kinetic energy of 10 MeV. Absolute differential value cross sections are obtained by normalizing the angle-integrated relative angular distribution to the N-P total cross section.
DOI: 10.17182/hepdata.25395.v1/t1
title: "Table 1" of "Nuclear Compton scattering from 12C and bound-nucleon polarizabilities"

description: No description provided.
description: SASK-LINAC. Nuclear compton scattering from C-12 and bound nucleon polarizabilities.
DOI: 10.17182/hepdata.25395.v1/t2
title: "Table 2" of "Nuclear Compton scattering from 12C and bound-nucleon polarizabilities"

description: C12* is 4.44 MeV state.
description: SASK-LINAC. Nuclear compton scattering from C-12 and bound nucleon polarizabilities.
DOI: 10.17182/hepdata.25396.v1/t1
title: "Table 1" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 0 to 5 PCT for 6 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t2
title: "Table 2" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 5 to 12 PCT for 6 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t3
title: "Table 3" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 12 to 23 PCT for 6 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t4
title: "Table 4" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 23 to 39 PCT for 6 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t5
title: "Table 5" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 39 to 81 PCT for 6 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t10
title: "Table 10" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 39 to 81 PCT for 8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t6
title: "Table 6" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 0 to 5 PCT for 8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t7
title: "Table 7" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 5 to 12 PCT for 8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t8
title: "Table 8" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 12 to 23 PCT for 8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t9
title: "Table 9" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 23 to 39 PCT for 8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t11
title: "Table 11" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 0 to 5 PCT for 10.8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t12
title: "Table 12" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 5 to 12 PCT for 10.8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t13
title: "Table 13" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 12 to 23 PCT for 10.8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t14
title: "Table 14" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 23 to 39 PCT for 10.8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25396.v1/t15
title: "Table 15" of "Proton emission in Au+Au collisions at 6, 8, and 10.8 GeV/nucleon"

description: The inverse slope, mean transverse mass and rapidity density values for centrality 39 to 77 PCT for 10.8 GeV/nucleon collisions. Statistical errors only.
description: BNL-AGS. Measurement of the transverse mass spectra of protons emitted in AU AU collisions at beam energies of 6, 8 and 10.8 GeV per nucleon. The data cover the rapidity range 0.5 to 1.5.
DOI: 10.17182/hepdata.25402.v1/t1
title: "Table 1" of "Systematics of the low-energy pionic double charge exchange in nuclei"

description: GST means nonanalog ground state.
description: PSI accelerator. Systematics of the low-energy pionic double charge exchange in nuclei.
DOI: 10.17182/hepdata.25402.v1/t2
title: "Table 2" of "Systematics of the low-energy pionic double charge exchange in nuclei"

description: GST means nonanalog ground state.
description: PSI accelerator. Systematics of the low-energy pionic double charge exchange in nuclei.
DOI: 10.17182/hepdata.25402.v1/t3
title: "Table 3" of "Systematics of the low-energy pionic double charge exchange in nuclei"

description: GST means nonanalog ground state.
description: PSI accelerator. Systematics of the low-energy pionic double charge exchange in nuclei.
DOI: 10.17182/hepdata.25402.v1/t4
title: "Table 4" of "Systematics of the low-energy pionic double charge exchange in nuclei"

description: GST means nonanalog ground state.
description: PSI accelerator. Systematics of the low-energy pionic double charge exchange in nuclei.
DOI: 10.17182/hepdata.25402.v1/t5
title: "Table 5" of "Systematics of the low-energy pionic double charge exchange in nuclei"

description: Data for double isobaric analog state. GST means nonanalog ground state.
description: PSI accelerator. Systematics of the low-energy pionic double charge exchange in nuclei.
DOI: 10.17182/hepdata.25403.v1/t1
title: "Table 1" of "Pion production in d p --&gt; d N pi"

description: Two first points on energy correspond to different luminosities.
description: CELSIUS accelerator.. Pion production in dp--& gt;dN pi reactions with deuteron projectiles.
DOI: 10.17182/hepdata.25404.v1/t1
title: "Table 1" 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 emittedon an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.22 &lt; ETARAP &lt; 2.5, is subdivided into eight nominally equal bins of 0.16 in pseudorapidity.
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/t2
title: "Table 2" 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 emittedon an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.38 &lt; ETARAP &lt; 2.34, is subdivided into eight nominally equal bins of 0.16 in pseudorapidity.
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/t3
title: "Table 3" 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 emittedon an event. The full ETARAP acceptance of the half-azimuth calorimeter, 1.54 &lt; ETARAP &lt; 2.18, is subdivided into eight nominally equal bins of 0.16 in pseudorapidity.
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/t4
title: "Table 4" 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 emittedon 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/t5
title: "Table 5" 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/t6
title: "Table 6" 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/t8
title: "Table 8" 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/t10
title: "Table 10" 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/t11
title: "Table 11" 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/t12
title: "Table 12" 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/t7
title: "Table 7" 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/t9
title: "Table 9" 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/t13
title: "Table 13" 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. 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/t15
title: "Table 15" 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. 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/t16
title: "Table 16" 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. 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/t14
title: "Table 14" 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. 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.