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NSR database version of April 24, 2024.

Search: Author = K.Hanold

Found 21 matches.

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2002SO06      Nucl.Phys. A705, 279 (2002)

G.A.Souliotis, W.Loveland, K.Hanold, G.J.Wozniak, D.J.Morrissey

Heavy Residue Formation in 20 MeV/nucleon 197Au + 90Zr Collisions

NUCLEAR REACTIONS 90Zr(197Au, X), E=20 MeV/nucleon; measured fragment yields, velocity distributions; deduced incomplete fusion, deep inelastic scattering. Comparison with model predictions.

doi: 10.1016/S0375-9474(02)00673-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1690.

2000FA21      Nucl.Phys. A679, 121 (2000)

T.S.Fan, K.X.Jing, L.Phair, K.Tso, M.McMahan, K.Hanold, G.J.Wozniak, L.G.Moretto

Excitation Functions and Mass Asymmetric Fission Barriers for Compound Nuclei 70, 76Se

NUCLEAR REACTIONS 12C(58Ni, X), (64Ni, X), E=6-14 MeV/nucleon; measured fragment charge distributions, production σ. 70,76Se deduced mass asymmetric fission barriers, transition state fission rates.

doi: 10.1016/S0375-9474(00)00334-1
Citations: PlumX Metrics

1999JI01      Nucl.Phys. A645, 203 (1999)

K.X.Jing, L.G.Moretto, A.C.Veeck, N.Colonna, I.Lhenry, K.Tso, K.Hanold, W.Skulski, Q.Sui, G.J.Wozniak

Transition State Rates and Mass Asymmetric Fission Barriers of Compound Nuclei 90, 94, 98Mo

NUCLEAR REACTIONS 12C(78Kr, X), (82Kr, X), (86Kr, X), E=6-13 MeV/nucleon; measured fragments σ(Z) vs E. 90,94,98Mo deduced mass asymmetric fission barriers, transition state fission rates.

doi: 10.1016/S0375-9474(98)00606-X
Citations: PlumX Metrics

1998SO11      Phys.Rev. C57, 3129 (1998)

G.A.Souliotis, K.Hanold, W.Loveland, I.Lhenry, D.J.Morrissey, A.C.Veeck, G.J.Wozniak

Heavy Residue Formation in 20 MeV/nucleon 197Au-12C and 197Au-27Al Collisions

NUCLEAR REACTIONS 12C, 27Al(197Au, X), E=20 MeV/nucleon; measured fragments isotopic yields vs momentum transfer, velocity distributions; deduced fission delay times. Comparison with statistical models. Fragment separator.

doi: 10.1103/PhysRevC.57.3129
Citations: PlumX Metrics

1995HA19      Phys.Rev. C52, 1462 (1995)

K.A.Hanold, D.Bazin, M.F.Mohar, L.G.Moretto, D.J.Morrissey, N.A.Orr, B.M.Sherrill, J.A.Winger, G.J.Wozniak, S.J.Yennello

Heavy Residues from Very Mass-Asymmetric Heavy-Ion Reactions

NUCLEAR REACTIONS 9Be, C, 27Al(129Xe, X), E=26-50 MeV/nucleon; measured fragment production σ, momenta for Z > 39. Boltzmann-Nordheim-Vlasov method, other data discussed.

doi: 10.1103/PhysRevC.52.1462
Citations: PlumX Metrics

1995OR02      Phys.Rev. C51, 3116 (1995)

N.A.Orr, N.Anantaraman, S.M.Austin, C.A.Bertulani, K.Hanold, J.H.Kelley, R.A.Kryger, D.J.Morrissey, B.M.Sherrill, G.A.Souliotis, M.Steiner, M.Thoennessen, J.S.Winfield, J.A.Winger, B.M.Young

Momentum Distributions of 9Li Fragments from the Breakup of 11Li and the Neutron Halo

NUCLEAR REACTIONS 9Be, 93Nb, 181Ta, 238U(11Li, 9LiX), E ≈ 66 MeV/nucleon; measured σ(θ(9Li)) vs momentum. 11Li deduced neutron halo characteristics. Energy-loss spectrometer.

doi: 10.1103/PhysRevC.51.3116
Citations: PlumX Metrics

1994JU01      Phys.Rev. C49, R5 (1994)

M.L.Justice, Y.Blumenfeld, N.Colonna, D.N.Delis, G.Guarino, K.Hanold, J.C.Meng, G.F.Peaslee, G.J.Wozniak, L.G.Moretto

Electromagnetic Dissociation of 238U at 120 MeV/nucleon

NUCLEAR REACTIONS U(9Be, F), (27Al, F), (Cu, F), (Ag, F), (238U, F), E=120 MeV/nucleon; measured fission σ, fragment velocities; deduced electromagnetic component estimate of fission σ.

doi: 10.1103/PhysRevC.49.R5
Citations: PlumX Metrics

1994MO34      Phys.Rev.Lett. 73, 3070 (1994)

C.P.Montoya, W.G.Lynch, D.R.Bowman, G.F.Peaslee, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, L.Phair, M.B.Tsang, J.B.Webster, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto

Fragmentation of Necklike Structures

NUCLEAR REACTIONS Cu(129Xe, X), E=49.8 MeV/nucleon; measured intermediate mass fragment yield vs velocity; deduced necklike structure role in emission.

doi: 10.1103/PhysRevLett.73.3070
Citations: PlumX Metrics

1993BA10      Nucl.Phys. A553, 749c (1993)

W.Bauer, D.R.Bowman, N.Carlin, N.Colonna, R.T.de Souza, C.K.Gelbke, W.G.Gong, K.Hanold, Y.D.Kim, M.A.Lisa, W.G.Lynch, M.A.McMahan, L.G.Moretto, G.F.Peaslee, L.Phair, M.B.Tsang, C.Williams, G.J.Wozniak, F.Zhu

Multifragment Emission in 36Ar + 197Au and 129Xe + 197Au Collisions

NUCLEAR REACTIONS 197Au(129Xe, X), E=50 MeV/nucleon; 197Au(36Ar, X), E=50-110 MeV/nucleon; measured intermediate mass fragments number, charged particle multiplicity. Model analysis.

doi: 10.1016/0375-9474(93)90692-Q
Citations: PlumX Metrics

1993BO16      Phys.Rev.Lett. 70, 3534 (1993)

D.R.Bowman, G.F.Peaslee, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto

Sources and Emission Time Scales in E/A = 50 MeV 129Xe + (nat)Cu Reactions

NUCLEAR REACTIONS Cu(129Xe, X), E=50 MeV/nucleon; measured (fragment)(fragment)(θ), velocity distributions; deduced source features, emission times.

doi: 10.1103/PhysRevLett.70.3534
Citations: PlumX Metrics

1993HA16      Phys.Rev. C48, 723 (1993)

K.Hanold, L.G.Moretto, G.F.Peaslee, G.J.Wozniak, D.R.Bowman, M.F.Mohar, D.J.Morrissey

Transition from Complete to Incomplete Fusion in Asymmetric Heavy Ion Reactions

NUCLEAR REACTIONS C, 27Al, Ti, Cu(129Xe, X), E=26, 31 MeV/nucleon; measured σ(fragment θ), (fragment)(fragment)-coin; deduced σ, source velocity. C, 27Al, Ti, Cu(139La, X), E=18 MeV/nucleon; calculated (fragment)(fragment)-coin, yield. Incomplete fusion model.

doi: 10.1103/PhysRevC.48.723
Citations: PlumX Metrics

1993PH01      Nucl.Phys. A564, 453 (1993)

L.Phair, D.R.Bowman, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, G.F.Peaslee, R.T.de Souza, M.B.Tsang, C.Williams, F.Zhu, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak

Azimuthal Correlations as a Test for Centrality in Heavy-Ion Collisions

NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; 197Au(129Xe, X), E=50 MeV/nucleon; measured (particle)(particle)(φ); deduced central collisions selectivity features.

doi: 10.1016/0375-9474(93)90515-Y
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1993RO02      Nucl.Phys. A551, 508 (1993)

P.Roussel-Chomaz, N.Colonna, Y.Blumenfeld, B.Libby, G.F.Peaslee, D.N.Delis, K.Hanold, M.A.McMahan, J.C.Meng, Q.C.Sui, G.J.Wozniak, L.G.Moretto, H.Madani, A.A.Marchetti, A.C.Mignerey, G.Guarino, N.Santoruvo, I.Iori, S.Bradley

Complex Fragment Production and Multifragmentation in 139La-Induced Reactions at 35, 40, 45 and 55 MeV/u

NUCLEAR REACTIONS 12C, 27Al, 40Ca, Cu, 139La(139La, X), E=35, 40, 45, 55 MeV/nucleon; measured σ(fragment E, θ), (fragment)(fragment)-coin; deduced source velocities, charge distributions.

doi: 10.1016/0375-9474(93)90460-F
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1992BO29      Phys.Rev. C46, 1834 (1992)

D.R.Bowman, C.M.Mader, G.F.Peaslee, W.Bauer, N.Carlin, R.T.de Souza, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto, W.A.Friedman

Intermediate Mass Fragment Emission as a Probe of Nuclear Dynamics

NUCLEAR REACTIONS 12C, 27Al, 51V, Cu, 89Y, 197Au(129Xe, X), E=50 MeV/nucleon; measured fragment muliplicity, charge distribution; deduced correlation with charged particle multiplicity, target independence. Hybrid model, dynamical emission aspects.

doi: 10.1103/PhysRevC.46.1834
Citations: PlumX Metrics

1992KE01      Nucl.Instrum.Methods Phys.Res. A311, 258 (1992)

W.L.Kehoe, A.C.Mignerey, A.Moroni, I.Iori, G.F.Peaslee, N.Colonna, K.Hanold, D.R.Bowman, L.G.Moretto, M.A.McMahan, J.T.Walton, G.J.Wozniak

A Modular Array to Detect Complex Fragments Produced in Intermediate-Energy Reverse-Kinematics Reactions

NUCLEAR REACTIONS 40Ca(139La, X), E=40 MeV/nucleon; Cu(129Xe, X), E=50 MeV/nucleon; measured fragment production vs Z, total charge for 2-, 3-, 4-fold events. 12C, 27Al, 51V, Cu(139La, X), E=40 MeV/nucleon; measured total charge for 2-, 3-, 4-fold events. Segmented silicon-silicon-plastic array.

doi: 10.1016/0168-9002(92)90871-Z
Citations: PlumX Metrics

1992OR03      Phys.Rev.Lett. 69, 2050 (1992)

N.A.Orr, N.Anantaraman, S.M.Austin, C.A.Bertulani, K.Hanold, J.H.Kelley, D.J.Morrissey, B.M.Sherrill, G.A.Souliotis, M.Thoennessen, J.S.Winfield, J.A.Winger

Momentum Distributions of 9Li Fragment Following the Breakup of 11Li

NUCLEAR REACTIONS 9Be, 93Nb, 181Ta(11Li, 9Li), E=66 MeV/nucleon; measured ejectile momentum distributions; deduced projectile extended neutron distribution role.

doi: 10.1103/PhysRevLett.69.2050
Citations: PlumX Metrics

1991BO30      Phys.Rev.Lett. 67, 1527 (1991)

D.R.Bowman, G.F.Peaslee, R.T.de Souza, N.Carlin, C.K.Gelbke, W.G.Gong, Y.D.Kim, M.A.Lisa, W.G.Lynch, L.Phair, M.B.Tsang, C.Williams, N.Colonna, K.Hanold, M.A.McMahan, G.J.Wozniak, L.G.Moretto, W.A.Friedman

Multifragment Disintegration of the 129Xe + 197Au System at E/A = 50 MeV

NUCLEAR REACTIONS 197Au(129Xe, X), E=50 MeV/nucleon; measured charged particle multiplicities. Dynamical, statistical models.

doi: 10.1103/PhysRevLett.67.1527
Citations: PlumX Metrics

1991DE22      Z.Phys. A339, 279 (1991)

D.N.Delis, Y.Blumenfeld, D.R.Bowman, N.Colonna, K.Hanold, K.Jing, M.Justice, J.C.Meng, G.F.Peaslee, G.J.Wozniak, L.G.Moretto

A Complete Ridge-Line Potential for Complex Fragment Emission

NUCLEAR REACTIONS 12C(63Cu, X), E=5-12.7 MeV/nucleon; measured σ vs fragment Z. 75Br deduced emission barriers, mass asymmetric fission, level density parameter ratio.

doi: 10.1007/BF01284065
Citations: PlumX Metrics

1991DE30      Nucl.Phys. A534, 403 (1991)

D.N.Delis, Y.Blumenfeld, D.R.Bowman, N.Colonna, K.Hanold, K.Jing, M.Justice, J.C.Meng, G.F.Peaslee, G.J.Wozniak, L.G.Moretto

Mass Asymmetric Fission Barriers for 75Br

NUCLEAR REACTIONS 12C(63Cu, X), E=5-12.7 MeV/nucleon; measured σ(fragment θ) spectra; deduced source velocities, charge distributions, σ(Z) vs E. 75Br deduced mass asymmetric fission barriers.

doi: 10.1016/0375-9474(91)90509-5
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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
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1988HA23      Phys.Rev. C38, 165 (1988); Erratum Phys.Rev. C38, 2465 (1988)

K.Hanold, D.J.Morrissey

High Energy γ Rays from the 12C + 12C and 40Ar + 48Ti Systems at 15 MeV/Nucleon

NUCLEAR REACTIONS 12C(12C, X), 48Ti(40Ar, X), E=15 MeV/nucleon; measured σ(θγ, Eθ); deduced source velocity.

doi: 10.1103/PhysRevC.38.165
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter K.Hanold: , K.A.HANOLD