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NSR database version of April 11, 2024.

Search: Author = J.Clayton

Found 20 matches.

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13990.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1342.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1098.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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