cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.22925.v1/t1
title: "Table 1" of "Charge exchange photoproduction of the a2- (1320) in association with Delta++ at 19.3-GeV/c"

description: No description provided.
description: SLAC-Hybrid Bubble Chamber. Study of charge exchange production of the A2(1320)- in association with the DEL++ at 19.3 GeV.
DOI: 10.17182/hepdata.22935.v1/t1
title: "Table 1" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t2
title: "Table 2" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t3
title: "Table 3" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t4
title: "Table 4" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t5
title: "Table 5" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t6
title: "Table 6" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22935.v1/t7
title: "Table 7" of "Analyzing power for pi- p charge exchange in the backward hemisphere from 301-MeV/c to 625-MeV/c and a test of pi N partial wave analyses"

description: Axis error includes +- 5/5 contribution (Uncertainty in background normalisation).
description: LAMPF. Measurement of the analysing power in pi- p charged exchange in the backward hemisphere from 301 to 625 MeV. Experiment uses a transversly polarized proton target.
DOI: 10.17182/hepdata.22936.v1/t1
title: "Table 1" of "Determination of electroweak parameters from the elastic scattering of muon-neutrinos and anti-neutrinos on electrons"

description: No description provided.
description: BNL-AGS. Determination of electroweak parameters from elastic scattering of muon neutrinos and antineutrinos on electrons.
DOI: 10.17182/hepdata.22936.v1/t2
title: "Table 2" of "Determination of electroweak parameters from the elastic scattering of muon-neutrinos and anti-neutrinos on electrons"

description: No description provided.
description: BNL-AGS. Determination of electroweak parameters from elastic scattering of muon neutrinos and antineutrinos on electrons.
DOI: 10.17182/hepdata.22936.v1/t3
title: "Table 3" of "Determination of electroweak parameters from the elastic scattering of muon-neutrinos and anti-neutrinos on electrons"

description: No description provided.
description: BNL-AGS. Determination of electroweak parameters from elastic scattering of muon neutrinos and antineutrinos on electrons.
DOI: 10.17182/hepdata.22937.v1/t1
title: "Table 1" of "Near-threshold photoproduction of $\Lambda(1520)$ from protons and deuterons"

description: The measured differential cross sections from the liquid hydrogen target, protons, as a function the K+ polar angle.
description: OSAKA. Measurement of the photoproduction of the LAMBDA(1520) baryon using liquid hydrogen and deuterium targets at photon energies below 2.4 GeV. The data were collected during 2002-2003 at the SPring-8 LEPS facility using a linearly polarized photon beam tagged in the energy range 1.5-2.4 GeV by detecting recoil electrons. Two charged tracks in the final state K+K-P from protons and K0K-P from neutrons were detected and the LAMBDA(1520) observed using missing mass (K+K+ and K+P modes) and invariant mass (K-P mode) techniques. Data are presented separately for each mode and using two methods of background subtraction, Monte-Carlo (MC) and sideband subtraction(SB). Numerical values supplied by Jia-Ye Chen.
DOI: 10.17182/hepdata.22937.v1/t2
title: "Table 2" of "Near-threshold photoproduction of $\Lambda(1520)$ from protons and deuterons"

description: The measured differential cross sections from the liquid hydrogen target, protons, as a function the photon energy at forward K+ polar angles of 19-43 degrees .
description: OSAKA. Measurement of the photoproduction of the LAMBDA(1520) baryon using liquid hydrogen and deuterium targets at photon energies below 2.4 GeV. The data were collected during 2002-2003 at the SPring-8 LEPS facility using a linearly polarized photon beam tagged in the energy range 1.5-2.4 GeV by detecting recoil electrons. Two charged tracks in the final state K+K-P from protons and K0K-P from neutrons were detected and the LAMBDA(1520) observed using missing mass (K+K+ and K+P modes) and invariant mass (K-P mode) techniques. Data are presented separately for each mode and using two methods of background subtraction, Monte-Carlo (MC) and sideband subtraction(SB). Numerical values supplied by Jia-Ye Chen.
DOI: 10.17182/hepdata.22937.v1/t3
title: "Table 3" of "Near-threshold photoproduction of $\Lambda(1520)$ from protons and deuterons"

description: The measured of differential cross section at backward K+/K0 polar angles of 120-150 degrees as a function of photon energy from the liquid hydrogen target, protons, and liquid deuterium target, deuterons.
description: OSAKA. Measurement of the photoproduction of the LAMBDA(1520) baryon using liquid hydrogen and deuterium targets at photon energies below 2.4 GeV. The data were collected during 2002-2003 at the SPring-8 LEPS facility using a linearly polarized photon beam tagged in the energy range 1.5-2.4 GeV by detecting recoil electrons. Two charged tracks in the final state K+K-P from protons and K0K-P from neutrons were detected and the LAMBDA(1520) observed using missing mass (K+K+ and K+P modes) and invariant mass (K-P mode) techniques. Data are presented separately for each mode and using two methods of background subtraction, Monte-Carlo (MC) and sideband subtraction(SB). Numerical values supplied by Jia-Ye Chen.
DOI: 10.17182/hepdata.22937.v1/t4
title: "Table 4" of "Near-threshold photoproduction of $\Lambda(1520)$ from protons and deuterons"

description: The measured of differential cross section at backward K+/K0 polar angles of 150-180 degrees as a function of photon energy from the liquid hydrogen target, protons, and liquid deuterium target, deuterons.
description: OSAKA. Measurement of the photoproduction of the LAMBDA(1520) baryon using liquid hydrogen and deuterium targets at photon energies below 2.4 GeV. The data were collected during 2002-2003 at the SPring-8 LEPS facility using a linearly polarized photon beam tagged in the energy range 1.5-2.4 GeV by detecting recoil electrons. Two charged tracks in the final state K+K-P from protons and K0K-P from neutrons were detected and the LAMBDA(1520) observed using missing mass (K+K+ and K+P modes) and invariant mass (K-P mode) techniques. Data are presented separately for each mode and using two methods of background subtraction, Monte-Carlo (MC) and sideband subtraction(SB). Numerical values supplied by Jia-Ye Chen.
DOI: 10.17182/hepdata.22938.v1/t1
title: "Table 1" of "Dimuon Production by Neutrinos in the {Fermilab} 15-ft. Bubble Chamber at the Tevatron"

description: No description provided.
description: QUADRUPOLE TRIPLET BEAM, NU TO NUBAR RATIO IS ABOUT 2.5, HE/NE MIXTURE AS THE TARGET.
DOI: 10.17182/hepdata.22938.v1/t2
title: "Table 2" of "Dimuon Production by Neutrinos in the {Fermilab} 15-ft. Bubble Chamber at the Tevatron"

description: No description provided.
description: QUADRUPOLE TRIPLET BEAM, NU TO NUBAR RATIO IS ABOUT 2.5, HE/NE MIXTURE AS THE TARGET.
DOI: 10.17182/hepdata.22938.v1/t3
title: "Table 3" of "Dimuon Production by Neutrinos in the {Fermilab} 15-ft. Bubble Chamber at the Tevatron"

description: No description provided.
description: QUADRUPOLE TRIPLET BEAM, NU TO NUBAR RATIO IS ABOUT 2.5, HE/NE MIXTURE AS THE TARGET.
DOI: 10.17182/hepdata.22938.v1/t4
title: "Table 4" of "Dimuon Production by Neutrinos in the {Fermilab} 15-ft. Bubble Chamber at the Tevatron"

description: No description provided.
description: QUADRUPOLE TRIPLET BEAM, NU TO NUBAR RATIO IS ABOUT 2.5, HE/NE MIXTURE AS THE TARGET.
DOI: 10.17182/hepdata.22990.v1/t1
title: "Table 1" of "Test of Scaling of the Massive Dihadron Cross Section"

description: No description provided.
description: FERMILAB. Study of massive di-hadron production in proton tungsten collisions at 800 GeV.. Numerical values supplied by D.Kaplan.
DOI: 10.17182/hepdata.22990.v1/t2
title: "Table 2" of "Test of Scaling of the Massive Dihadron Cross Section"

description: Triple differential cross section. Note that the errors plotted in the original figure are 2 time too large. The numbers given here are correct.
description: FERMILAB. Study of massive di-hadron production in proton tungsten collisions at 800 GeV.. Numerical values supplied by D.Kaplan.
DOI: 10.17182/hepdata.22991.v1/t1
title: "Table 1" of "A MEASUREMENT OF THE TOTAL HADRONIC CROSS-SECTION IN TAGGED gamma gamma REACTIONS"

description: Errors are statistical only.
description: SLAC-PEP. Measurement of the total hadronic cross-section for virtual photon-photon interactions at centre-of-mass energies from 2 to 10 GeV. Cross-section extrapolated to Q**2 = 0 using the generalised vector dominance model.
DOI: 10.17182/hepdata.22991.v1/t2
title: "Table 2" of "A MEASUREMENT OF THE TOTAL HADRONIC CROSS-SECTION IN TAGGED gamma gamma REACTIONS"

description: Errors are statistical only.
description: SLAC-PEP. Measurement of the total hadronic cross-section for virtual photon-photon interactions at centre-of-mass energies from 2 to 10 GeV. Cross-section extrapolated to Q**2 = 0 using the generalised vector dominance model.
DOI: 10.17182/hepdata.22991.v1/t3
title: "Table 3" of "A MEASUREMENT OF THE TOTAL HADRONIC CROSS-SECTION IN TAGGED gamma gamma REACTIONS"

description: Errors are statistical only.
description: SLAC-PEP. Measurement of the total hadronic cross-section for virtual photon-photon interactions at centre-of-mass energies from 2 to 10 GeV. Cross-section extrapolated to Q**2 = 0 using the generalised vector dominance model.
DOI: 10.17182/hepdata.22991.v1/t4
title: "Table 4" of "A MEASUREMENT OF THE TOTAL HADRONIC CROSS-SECTION IN TAGGED gamma gamma REACTIONS"

description: Errors are statistical only.
description: SLAC-PEP. Measurement of the total hadronic cross-section for virtual photon-photon interactions at centre-of-mass energies from 2 to 10 GeV. Cross-section extrapolated to Q**2 = 0 using the generalised vector dominance model.
DOI: 10.17182/hepdata.22998.v1/t1
title: "Table 1" of "The Production of $J/_{\psi}$ and Associated Particles in the Collision of 530 GeV/c Protons and Pions with Nuclear Targets"

description: Interacting beam cross-section.
description: PLAB=530 GEV. A DEPENDENCE OF J/PSI PRODUCTION AT THE FERMILAB TEVATRON.
DOI: 10.17182/hepdata.22998.v1/t2
title: "Table 2" of "The Production of $J/_{\psi}$ and Associated Particles in the Collision of 530 GeV/c Protons and Pions with Nuclear Targets"

description: No description provided.
description: PLAB=530 GEV. A DEPENDENCE OF J/PSI PRODUCTION AT THE FERMILAB TEVATRON.
DOI: 10.17182/hepdata.22998.v1/t3
title: "Table 3" of "The Production of $J/_{\psi}$ and Associated Particles in the Collision of 530 GeV/c Protons and Pions with Nuclear Targets"

description: No description provided.
description: PLAB=530 GEV. A DEPENDENCE OF J/PSI PRODUCTION AT THE FERMILAB TEVATRON.
DOI: 10.17182/hepdata.22999.v1/t1
title: "Table 1" of "K0(S) PRODUCTION IN ANTI-P P INTERACTIONS AT S**(1/2) = 630-GeV AND 1800-GEV"

description: Estimated effective cross sections for events which pass the trigger and selection criteria. The uncertainties in these represent the principal source of error in the overall normalisation of the results.
description: FNAL-Tevatron Collider. Measurement of inclusive transverse momentum spectra for K0S mesons produced in 630 and 1800 GeV (pbar p) centre-of-mass energy collisions by the CDF Collaboration.. Numerical values supplied by L.Galtieri.
DOI: 10.17182/hepdata.22999.v1/t2
title: "Table 2" of "K0(S) PRODUCTION IN ANTI-P P INTERACTIONS AT S**(1/2) = 630-GeV AND 1800-GEV"

description: Statistical errors only.
description: FNAL-Tevatron Collider. Measurement of inclusive transverse momentum spectra for K0S mesons produced in 630 and 1800 GeV (pbar p) centre-of-mass energy collisions by the CDF Collaboration.. Numerical values supplied by L.Galtieri.
DOI: 10.17182/hepdata.22999.v1/t4
title: "Table 4" of "K0(S) PRODUCTION IN ANTI-P P INTERACTIONS AT S**(1/2) = 630-GeV AND 1800-GEV"

description: Mean values of various quantities.
description: FNAL-Tevatron Collider. Measurement of inclusive transverse momentum spectra for K0S mesons produced in 630 and 1800 GeV (pbar p) centre-of-mass energy collisions by the CDF Collaboration.. Numerical values supplied by L.Galtieri.
DOI: 10.17182/hepdata.22999.v1/t3
title: "Table 3" of "K0(S) PRODUCTION IN ANTI-P P INTERACTIONS AT S**(1/2) = 630-GeV AND 1800-GEV"

description: Statistical errors only.
description: FNAL-Tevatron Collider. Measurement of inclusive transverse momentum spectra for K0S mesons produced in 630 and 1800 GeV (pbar p) centre-of-mass energy collisions by the CDF Collaboration.. Numerical values supplied by L.Galtieri.
DOI: 10.17182/hepdata.23000.v1/t1
title: "Table 1" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: Corrected Cross Sections (Lund MC used to extrapolate).
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23000.v1/t2
title: "Table 2" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: R value for K0 production.
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23000.v1/t3
title: "Table 3" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: K0 differential cross section as function of the fractional energy.
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23000.v1/t4
title: "Table 4" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: K0 differential cross section as function of rapidity for the total 291 inverse pb HRS data.
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23000.v1/t5
title: "Table 5" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: Rapidity distributions for charm quark (D*) tagged events.
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23000.v1/t6
title: "Table 6" of "QUARK HADRONIZATION PROBED BY K0 MESONS"

description: Rapidity distributions for the light quark tagged events.
description: SLAC-PEP. HRS Collaboration. Measurement of total and differential K0 cross sections from e+ e- collisions at sqrt(s) = 29 GeV. Data are tagged as charm quark and light quark events and the distributions compared, along with the distributions for all charged particles. The charm quark tagging requires the observation of a D*0 --& gt; D0 PI+ decay where the D0 decays into either K- PI+, K- PI+ PI- PI+ or K- PI+ PI0. For the K PI and K 2PI modes Z & lt; 0.4 and for the K 3PI Z & lt; 0.6. The light quark tagging requires one charged particle in the event to have momentum fraction X(=2p/sqrt(s)) & gt; 0.65 (i.e. p & gt; 9.43 GeV). These data supercede and add to that presented in Kesten et al., PL 161B (85) 412.
DOI: 10.17182/hepdata.23001.v1/t1
title: "Table 1" of "Proton proton bremsstrahlung at 280-MeV"

description: Estimated scale uncertainty is 1.5 pct.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t2
title: "Table 2" of "Proton proton bremsstrahlung at 280-MeV"

description: Estimated scale uncertainty is 1.5 pct.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t3
title: "Table 3" of "Proton proton bremsstrahlung at 280-MeV"

description: Estimated scale uncertainty is 1.5 pct.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t4
title: "Table 4" of "Proton proton bremsstrahlung at 280-MeV"

description: Estimated scale uncertainty is 1.5 pct.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t6
title: "Table 6" of "Proton proton bremsstrahlung at 280-MeV"

description: Values include an arbitrary rescaling factor of 0.667.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t5
title: "Table 5" of "Proton proton bremsstrahlung at 280-MeV"

description: Values include an arbitrary rescaling factor of 0.667.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.
DOI: 10.17182/hepdata.23001.v1/t7
title: "Table 7" of "Proton proton bremsstrahlung at 280-MeV"

description: Values include an arbitrary rescaling factor of 0.667.
description: TRIUMF. Measurement of proton proton bremsstrahlung with polarized proton beam at 280 MeV kinetic energy. Because the detection system of the two protons differs, a distinction is made between the one on the same side as the photon (LE) and the one on the opposite side (HE). In the notation here particle 3 is the photon, particle 4 the LE proton, and particle 5 the HE proton.