NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = J.Clayton Found 20 matches. 1995BE69 Nucl.Instrum.Methods Phys.Res. B99, 505 (1995) J.Bendahan, J.Clayton, K.Frankhauser, T.Gozani, J.Krivicich, R.Loveman, E.Pentaleri, P.Ryge, P.Sawa, J.Stevenson Measurements and Analysis of Carbon and Oxygen Neutron Inelastic Cross Sections below 10 MeV NUCLEAR REACTIONS 12C, 16O(n, n'γ), E=6.2-8.51 MeV; measured σ(θ). Inconsistencies, errors in neutron σ libraries.
doi: 10.1016/0168-583X(94)00748-9
1993LU01 Phys.Rev. C47, 1211 (1993) S.J.Luke, R.Vandenbosch, W.Benenson, J.Clayton, K.Joh, D.Krofcheck, T.K.Murakami, J.D.Stevenson High Energy γ Rays from 14N + (nat)Ag at 35 MeV/nucleon NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(θ, Eγ), high energy γ(θ). Nucleon exchange transport model, diffuse momentum distribution.
doi: 10.1103/PhysRevC.47.1211
1993PF01 Z.Phys. A347, 67 (1993) R.Pfaff, B.M.Young, W.Benenson, J.Clayton, D.J.Morrissey, N.A.Orr, T.Reposeur, M.Thoennessen, J.A.Winger Target Isotope Effect in High Energy Photon Production at E/A = 10 MeV NUCLEAR REACTIONS, ICPND 112,124Sn(12C, X), E=10 MeV/nucleon; measured Eγ, Iγ, photon yield vs Eγ; deduced σ ratio. Neutron-Proton bremsstrahlung model.
doi: 10.1007/BF01301279
1992CL02 Phys.Rev. C45, 1810 (1992) J.Clayton, W.Benenson, M.Cronqvist, R.Fox, D.Krofcheck, R.Pfaff, T.Reposeur, J.D.Stevenson, J.S.Winfield, B.Young, M.F.Mohar, C.Bloch, D.E.Fields Proton-Deuteron Bremsstrahlung at 145 and 195 MeV NUCLEAR REACTIONS 2H(p, γ), E=145, 195 MeV; measured Eγ, Iγ, σ(θ, Eγ); deduced n-p bremsstrahlung σ. BaF detectors.
doi: 10.1103/PhysRevC.45.1810
1992CL03 Phys.Rev. C45, 1815 (1992) J.Clayton, W.Benenson, M.Cronqvist, R.Fox, D.Krofcheck, R.Pfaff, T.Reposeur, J.D.Stevenson, J.S.Winfield, B.Young, M.F.Mohar, C.Bloch, D.E.Fields High Energy Gamma Ray Production in Proton-Induced Reactions at 104, 145, and 195 MeV NUCLEAR REACTIONS C, Zn, Pb(p, γ), E=104, 145, 195 MeV; measured Eγ, σ(θ, Eγ); deduced reaction mechanism, proton-neutron collision associated γ-emission probability.
doi: 10.1103/PhysRevC.45.1815
1992RE01 Phys.Lett. 276B, 418 (1992) T.Reposeur, J.Clayton, W.Benenson, M.Cronqvist, S.Hannuschke, S.Howden, J.Karn, D.Krofcheck, A.Nadasen, C.Ogilvie, R.Pfaff, J.D.Stevenson, A.Vander Molen, G.D.Westfall, K.Wilson, J.S.Winfield, B.Young, M.F.Mohar, D.J.Morrissey Impact Parameter Dependence of High Energy Gamma Ray Production in Heavy-Ion Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=65 MeV/nucleon; measured σ(fragment θ, Eγ), (fragment)γ-coin; deduced impact parameter dependence. Multi-detector array.
doi: 10.1016/0370-2693(92)91660-2
1990CL04 Phys.Rev. C42, 1009 (1990) J.Clayton, J.Stevenson, W.Benenson, D.Krofcheck, D.J.Morrissey, T.K.Murakami, J.S.Winfield Search for Photons from the Decay of the Delta Resonance in Heavy-Ion Collisions NUCLEAR REACTIONS Zn(14N, X), E=75 MeV/nucleon; measured σ(Eγ, θγ); deduced no Δ-resonance decay related photons.
doi: 10.1103/PhysRevC.42.1009
1990OG03 Phys.Rev. C42, R10 (1990) C.A.Ogilvie, W.Bauer, D.A.Cebra, J.Clayton, S.Howden, J.Karn, A.Nadasen, A.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield Disappearance of Flow and Its Relevance to Nuclear Matter Physics NUCLEAR REACTIONS 51V(40Ar, X), E=35, 45, 55, 65, 75, 85 MeV/nucleon; measured transverse collective motion in light particles (Z=1, 2, 3); deduced E(balance) lower limit, nuclear meanfield component features.
doi: 10.1103/PhysRevC.42.R10
1990WI03 Phys.Rev. C41, R1881 (1990) W.K.Wilson, W.Benenson, D.A.Cebra, J.Clayton, S.Howden, J.Karn, T.Li, C.A.Ogilvie, A.Vander Molen, G.D.Westfall, J.S.Winfield, B.Young, A.Nadasen Azimuthal Asymmetry in Ar + V Collisions from E/A = 35 to 85 MeV NUCLEAR REACTIONS 51V(40Ar, X), E=35-85 MeV/nucleon; measured σ(fragment θ); deduced asymmetry mechanism.
doi: 10.1103/PhysRevC.41.R1881
1989CL05 Phys.Rev. C40, 1207 (1989) J.Clayton, J.Stevenson, W.Benenson, Y.Chen, E.Kashy, A.R.Lampis, M.Samuel, C.L.Tam, M.F.Mohar, D.J.Morrissey, T.K.Murakami, B.Sherrill, J.S.Winfield High Energy Gamma-Ray Production in the Heavy-Ion Reaction 136Xe + Sn at E/A = 89 and 124 MeV NUCLEAR REACTIONS Sm(136Xe, X), E=89, 124 MeV/nucleon; measured σ(Eγ, θγ); deduced high energy γ-emission mechanism.
doi: 10.1103/PhysRevC.40.1207
1989MU11 Phys.Rev. C40, 2079 (1989) T.K.Murakami, W.Benenson, Y.Chen, J.Clayton, E.Kashy, J.Stevenson, C.L.Tam, K.Hanold, M.Mohar High-Energy Gamma Rays from Reactions Induced by E/A = 15 MeV Heavy-Ion Beams NUCLEAR REACTIONS Zr(86Kr, X), (40Ar, X), Ca(40Ar, X), E=15 MeV/nucleon; measured σ(Eγ, θγ), γ-multiplicity; deduced γ-emission source velocity.
doi: 10.1103/PhysRevC.40.2079
1989OG02 Phys.Rev. C40, 654 (1989) C.A.Ogilvie, D.A.Cebra, J.Clayton, S.Howden, J.Karn, A.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield Determination of the Impact Vector in Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=40-100 MeV/nucleon; calculated particle multiplicity, midrapidity charge. 12C(12C, X), E=50 MeV/nucleon; analyzed σ(fragment E, θ), Z=2. 51V(40Ar, X), E=35 MeV/nucleon; calculated midrapidity charge yields.
doi: 10.1103/PhysRevC.40.654
1989OG03 Phys.Rev. C40, 2592 (1989) C.A.Ogilvie, D.A.Cebra, J.Clayton, P.Danielewicz, S.Howden, J.Karn, A.Nadasen, A.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield Transverse Collective Motion in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=35 MeV/nucleon; 12C(12C, X), E=50 MeV/nucleon; measured light charged particle fragment rapidities; deduced reaction mechanism, transverse collective motion evidence.
doi: 10.1103/PhysRevC.40.2592
1989OG04 Phys.Lett. 231B, 35 (1989) C.A.Ogilvie, D.A.Cebra, J.Clayton, P.Danielewicz, S.Howden, J.Karn, A.Nadasen, A.Vander Molen, G.D.Westfall, W.K.Wilson, J.S.Winfield Longitudinal Collective Motion in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 51V(40Ar, X), E=35 MeV/nucleon; 12C(12C, X), E=50 MeV/nucleon; measured light charged particles; deduced collective motion longitudinal component.
doi: 10.1016/0370-2693(89)90108-1
1989TA10 Phys.Rev. C39, 1371 (1989) C.L.Tam, J.Stevenson, W.Benenson, J.Clayton, Y.Chen, E.Kashy, A.R.Lampis, D.J.Morrissey, M.Samuel, T.K.Murakami, J.S.Winfield Mass Dependence of High-Energy Gamma-Ray Production in Heavy-Ion Reactions NUCLEAR REACTIONS Li, Pb(7Li, X), Mg(20Ne, X), Pb, Ca(40Ar, X), E=30 MeV/nucleon; measured σ(E(γ), θ(γ)); deduced reaction mechanism, γ production σ.
doi: 10.1103/PhysRevC.39.1371
1988LA20 Phys.Rev. C38, 1961 (1988) A.R.Lampis, J.Stevenson, W.Benenson, J.Clayton, D.Cebra, Y.Chen, D.Fox, E.Kashy, D.J.Morrissey, M.Samuel, R.Smith, C.L.Tam, G.D.Westfall, K.Wilson, J.S.Winfield Correlations between High-Energy Gamma Rays and Light Fragments in Heavy Ion Collisions NUCLEAR REACTIONS Zn(14N, pγ), (14N, dγ), (14N, tγ), E=40 MeV/nucleon; measured (particle)γ-coin, σ(Ep, θp, θγ).
doi: 10.1103/PhysRevC.38.1961
1988MO18 Phys.Rev. C38, 737 (1988) M.F.Mohar, E.Adamides, W.Benenson, C.Bloch, B.A.Brown, J.Clayton, E.Kashy, M.Lowe, J.A.Nolen, Jr., W.E.Ormand, J.van der Plicht, B.Sherrill, J.Stevenson, J.S.Winfield Mass of 39Sc via the 40Ca(7Li, 8He) Reaction NUCLEAR REACTIONS 40Ca(7Li, 8He), E=27.24 MeV/nucleon; measured σ(E(8He)); deduced Q, mass equation parameters. 39Sc deduced mass excess. Isobaric multiplet mass equation, isospin-nonconserving Hamiltonian.
doi: 10.1103/PhysRevC.38.737
1988ST06 Phys.Rev. C37, 2220 (1988) J.Stevenson, B.A.Brown, Y.Chen, J.Clayton, E.Kashy, D.Mikolas, J.Nolen, M.Samuel, B.Sherrill, J.S.Winfield, Z.Q.Xie, R.E.Julies, W.A.Richter Search for the Exotic Nucleus 10He NUCLEAR REACTIONS Sn(18O, X), E=30 MeV/nucleon; measured fragment mass spectra; deduced 10He production upper limit. NUCLEAR STRUCTURE 4,5,6,7,8,9,10He; calculated binding energy. Shell model.
doi: 10.1103/PhysRevC.37.2220
1988TA22 Phys.Rev. C38, 2526 (1988) C.L.Tam, J.Stevenson, W.Benenson, J.Clayton, Y.Chen, E.Kashy, A.R.Lampis, D.J.Morrissey, M.Samuel, T.K.Murakami, J.S.Winfield High-Energy Gamma-Ray Production in Light-Ion Induced Reactions NUCLEAR REACTIONS C, Zn, Pb(p, X), E=53 MeV/nucleon; C, Zn, Pb(α, X), E=25, 53 MeV/nucleon; measured σ(θγ, Eγ); deduced γ-production mechanism.
doi: 10.1103/PhysRevC.38.2526
1986ST07 Phys.Rev.Lett. 57, 555 (1986) J.Stevenson, K.B.Beard, W.Benenson, J.Clayton, E.Kashy, A.Lampis, D.J.Morrissey, M.Samuel, R.J.Smith, C.L.Tam, J.S.Winfield High-Energy Gamma-Ray Emission in Heavy-Ion Collisions NUCLEAR REACTIONS Pb, Zn, C(14N, X), E=20, 30, 40 MeV/nucleon; measured Eγ, Iγ, γ(θ); deduced model parameters. Individual neutron-proton collision induced bremsstrahlung.
doi: 10.1103/PhysRevLett.57.555
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