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Search: Author = J.R.Huizenga

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1993WI07      Phys.Rev. C47, 2135 (1993)

J.L.Wile, S.S.Datta, W.U.Schroder, J.Toke, D.Pade, S.P.Baldwin, J.R.Huizenga, B.M.Quednau, R.T.deSouza, B.M.Szabo

Thermal Characteristics of Composite Systems Formed in Fusion of 28Si with 118Sn and 124Sn Nuclei

NUCLEAR REACTIONS 118,124Sn(28Si, X), E=120-150 MeV; measured n(evaporation residue)-coin, neutron multiplicities. 146,152Gd deduced decay pattern differences. Statistical model effective level density parameters.

doi: 10.1103/PhysRevC.47.2135
Citations: PlumX Metrics

1991CH41      Phys.Rev. C44, R2249 (1991)

M.B.Chatterjee, S.P.Baldwin, J.R.Huizenga, D.Pade, B.M.Quednau, W.U.Schroder, B.M.Szabo, J.Toke

Energy Partition in Near-Barrier Strongly Damped Collisions 58Ni + 208Pb

NUCLEAR REACTIONS 58Ni(208Pb, xn), E=6.65 MeV/nucleon; measured exclusive n(fragment)-coin; deduced excitation energy division between two massive projectile-, target-like reaction products, appreciable Pb-like donor-fragments heating in net mass transfer reaction channels.

doi: 10.1103/PhysRevC.44.R2249
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1991TO04      Phys.Rev. C44, 390 (1991)

J.Toke, R.Planeta, W.U.Schroder, J.R.Huizenga

Correlations Between Energy and Mass Partition in the Damped Reaction 165Ho + 74Ge at E(lab) = 8.5 MeV/Nucleon

NUCLEAR REACTIONS 74Ge(165Ho, X), E=8.5 MeV/nucleon; analyzed data; deduced excitation energy division, mass asymmetry correlations, energy loss dependence, heat generation isospin symmetry.

doi: 10.1103/PhysRevC.44.390
Citations: PlumX Metrics

1990TO06      Nucl.Instrum.Methods Phys.Res. A288, 406 (1990)

J.Toke, W.U.Schroder, J.R.Huizenga

Aspects of Kinematical Coincidence Measurements of Excitation Energy Division in Damped Reactions

NUCLEAR REACTIONS 165Ho(56Fe, X), E=505 MeV; analyzed (fragment)(fragment)-correlation; deduced finite resolution induced systematic errors. Kinematical coincidence setup.

doi: 10.1016/0168-9002(90)90131-O
Citations: PlumX Metrics

1989DE01      Phys.Rev. C39, 114 (1989)

R.T.de Souza, W.U.Schroder, J.R.Huizenga, J.Toke, S.S.Datta, J.L.Wile

Nucleon Exchange in the Absence of Strong Driving Forces: The reaction 238U + 48Ca at E(lab) = 425 MeV

NUCLEAR REACTIONS 238U(48Ca, X), E=8.5 MeV/nucleon; measured σ(fragment θ), mass, charge, energy distributions; deduced mass, Z moments.

doi: 10.1103/PhysRevC.39.114
Citations: PlumX Metrics

1989HU08      Phys.Rev. C40, 668 (1989)

J.R.Huizenga, A.N.Behkami, I.M.Govil, W.U.Schroder, J.Toke

Influence of Rotation-Induced Nuclear Deformation on α-Particle Evaporation Spectra

NUCLEAR REACTIONS 63Cu(α, α), E ≈ 5-20 MeV; calculated transmission coefficient vs E, L. 27Al(40Ar, X), E=190 MeV; 64Ni(19F, X), E=120 MeV; 27Al(32S, X), E=100-150 MeV; calculated α-spectra. Statistical model.

doi: 10.1103/PhysRevC.40.668
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1989TO10      Phys.Rev. C40, R1577 (1989)

J.Toke, W.U.Schroder, J.R.Huizenga

Correlations between Fragment Mass and Excitation Energy in Damped Reactions

NUCLEAR REACTIONS 56Fe(165Ho, X), E=505 MeV; analyzed data. Monte Carlo simulations.

doi: 10.1103/PhysRevC.40.R1577
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1989WI10      Phys.Rev. C39, 1845 (1989)

J.L.Wile, S.S.Datta, W.U.Schroder, J.R.Huizenga, J.Toke, R.T.de Souza

Nonequilibrium Effects in the 139La + 40Ar Reaction at 10 MeV per Nucleon Observed in a Study of Neutron Emission

NUCLEAR REACTIONS 139La(40Ar, nX), E=400 MeV; measured σ(En, θn) in coincidence with fragment; deduced excitation energy division, preequilibrium emission of neutrons.

doi: 10.1103/PhysRevC.39.1845
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1989WI17      Phys.Rev. C40, 1700 (1989)

J.L.Wile, S.S.Datta, W.U.Schroder, J.R.Huizenga, R.T.de Souza, D.Pade

Excitation Energy Equilibration in Damped 139La + 40Ar Collisions at 15 MeV per Nucleon

NUCLEAR REACTIONS 139La(40Ar, X), E=600 MeV; measured (fragment n)-coin, σ(En, θn). One-body nucleon exchange model analysis.

doi: 10.1103/PhysRevC.40.1700
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1989WI21      Phys.Rev.Lett. 63, 2551 (1989)

J.L.Wile, S.S.Datta, R.T.de Souza, J.R.Huizenga, D.Pade, W.U.Schroder, J.Toke

Evidence for Radial-Energy Scaling of Nonequilibrium Neutron Yield in Damped 139La + 40Ar Reactions

NUCLEAR REACTIONS 139La(40Ar, xn), E=400, 600 MeV; measured neutron multiplicity vs total kinetic energy loss; other data analyzed; deduced angular momentum dependence vs energy loss. Stochastic nucleon exchange model.

doi: 10.1103/PhysRevLett.63.2551
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1988DE13      Phys.Rev. C37, 1783 (1988)

R.T.de Souza, W.U.Schroder, J.R.Huizenga, R.Planeta, K.Kwiatkowski, V.E.Viola, H.Breuer

Evolution of Mass and Charge Asymmetry in Damped Heavy-Ion Reactions

NUCLEAR REACTIONS 238U(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=8.5 MeV/nucleon; measured fragment spectra; deduced fragment Z, N first, second moments.

doi: 10.1103/PhysRevC.37.1783
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1988DE15      Phys.Rev. C37, 1901 (1988)

R.T.de Souza, J.R.Huizenga, W.U.Schroder

Effect of a Steep Gradient in the Potential Energy Surface on Nucleon Exchange

NUCLEAR REACTIONS 238U(40Ca, X), E=340 MeV; measured σ(fragment θ) vs energy loss, mass number, atomic number, energy distributions; deduced charge, mass distributions, first, second moments, associated correlations.

doi: 10.1103/PhysRevC.37.1901
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1988PL01      Phys.Rev. C38, 195 (1988)

R.Planeta, S.H.Zhou, K.Kwiatkowski, W.G.Wilson, V.E.Viola, H.Breuer, D.Benton, F.Khazaie, R.J.McDonald, A.C.Mignerey, A.Weston-Dawkes, R.T.de Souza, J.R.Huizenga, W.U.Schroder

N/Z Equilibration in Damped Collisions Induced by E/A = 8.5 MeV 58Ni and 64Ni on 238U

NUCLEAR REACTIONS 238U(58Ni, X), (64Ni, X), E=8.5 MeV/nucleon; measured projectile fragment yields; deduced centroids, variances, correlation coefficients.

doi: 10.1103/PhysRevC.38.195
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1987GO32      Phys.Lett. 197B, 515 (1987)

I.M.Govil, J.R.Huizenga, W.U.Schroder, J.Toke

Shapes of α-Particle Spectra from Energetic Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS 27Al(40Ar, X), E=190 MeV; analyzed σ(θ, Eα) following fusion. Statistical model.

doi: 10.1016/0370-2693(87)91046-X
Citations: PlumX Metrics

1987WI05      Phys.Rev. C35, 1608 (1987)

J.L.Wile, W.U.Schroder, J.R.Huizenga, D.Hilscher

Temperature, Energies, and Degree of Thermal Equilibration of Fragments in Damped Nuclear Reactions

NUCLEAR REACTIONS 165Ho(56Fe, X), (56Fe, xn), E not given; calculated neutron multiplicities, spectral slope parameters; deduced fragment equilibrium characteristics.

doi: 10.1103/PhysRevC.35.1608
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1986BU17      Phys.Rev. C34, 2016 (1986)

M.A.Butler, S.S.Datta, R.T.de Souza, J.R.Huizenga, W.U.Schroder, J.Toke, J.L.Wile

Relaxation of the Mass-Asymmetry Degree of Freedom In Heavy-Ion Reactions

NUCLEAR REACTIONS 58Ni(165Ho, X), E=970, 1075 MeV; measured σ(fragment, θ) vs mass, E; deduced mass asymmetry degree of freedom relaxation. Position sensitive multiwire avalanche.

doi: 10.1103/PhysRevC.34.2016
Citations: PlumX Metrics

1986RO02      Phys.Rev. C33, 560 (1986)

H.Rossner, J.R.Huizenga, W.U.Schroder

Fission Fragment Angular Distributions

NUCLEAR REACTIONS 208Pb(32S, F), E=180, 210 MeV; 208Pb(28Si, F), E=160-260 MeV; 208Pb(24Mg, F), (19F, F), 209Bi(α, F), E not given; analyzed fission fragment σ(E, θ); deduced model parameters. Statistical scission model.

doi: 10.1103/PhysRevC.33.560
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1985TU01      Phys.Rev. C32, 214 (1985)

L.E.Tubbs, J.R.Birkelund, J.R.Huizenga, D.Hilscher, U.Jahnke, H.Rossner, B.Gebauer

Linear Momentum Transfer in 292-MeV 20Ne-Induced Fission of 165Ho, 181Ta, 197Au, 209Bi, and 238U

NUCLEAR REACTIONS 165Ho, 181Ta, 197Au, 209Bi, 238U(20Ne, F), E=292 MeV; measured fission (fragment)(fragment)(θ), (fragment)(fragment)(φ). 185Ir, 201Bi, 217Ac, 229Np, 258No deduced linear momentum transfer.

doi: 10.1103/PhysRevC.32.214
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1984BI06      Phys.Rev. C30, 401 (1984)

J.R.Birkelund, J.R.Huizenga

Measurement of Nuclear Potentials from Fusion Excitation Functions

NUCLEAR REACTIONS 27Al(20Ne, X), E(cm) ≈ 16-200 MeV; calculated fusion σ(E); deduced critical distance model limitations in potential parameter determination.

doi: 10.1103/PhysRevC.30.401
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1984MI01      Phys.Rev. C29, 158 (1984)

A.C.Mignerey, K.L.Wolf, D.G.Raich, V.E.Viola, Jr., J.R.Birkelund, W.U.Schroder, J.R.Huizenga

Bombarding Energy Dependence of the 144Sm + 84Kr Reaction

NUCLEAR REACTIONS 144Sm(84Kr, X), E=470, 595, 720 MeV; measured σ(fragment E, θ, Z), total kinetic energy loss; deduced large exit channel deformations, orbiting probability.

doi: 10.1103/PhysRevC.29.158
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1984RO13      Phys.Rev.Lett. 53, 38 (1984)

H.H.Rossner, J.R.Huizenga, W.U.Schroder

Statistical Scission Model of Fission-Fragment Angular Distributions

NUCLEAR REACTIONS 238U(40Ar, F), E=340 MeV; 238U(16O, F), E=114, 140 MeV; 208Pb(32S, F), E=210-266 MeV; 208Pb(28Si, F), E=180-240 MeV; 208Pb(24Mg, F), E=145-190 MeV; 209Bi(16O, F), E=112, 134 MeV; 208Pb(19F, F), E=120-170 MeV; 197Au(22Ne, F), E=154-190 MeV; 192Os(16O, F), E=140 MeV; 198Pt(12C, F), E=186 MeV; calculated fission fragment σ(θ)/σ(90°). Statistical scission model.

doi: 10.1103/PhysRevLett.53.38
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1983BI02      Phys.Rev. C27, 882 (1983)

J.R.Birkelund, A.D.Hoover, J.R.Huizenga, W.U.Schroder, W.W.Wilcke

Fusion Cross Sections for the 165Ho + 56Fe Reaction

NUCLEAR REACTIONS 165Ho(56Fe, X), (56Fe, F), E=351, 421, 462, 510 MeV; measured fusion, fission σ(fragment θ); deduced σ(fusion) vs E. Dynamical model analysis. 165Ho(40Ar, X), E(cm) ≈ 150-300 MeV; 165Ho(84Kr, X), E(cm) ≈ 300-450 MeV; analyzed σ(fusion) vs E. Dynamical model.

doi: 10.1103/PhysRevC.27.882
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1983BI13      Ann.Rev.Nucl.Part.Sci. 33, 265 (1983)

J.R.Birkelund, J.R.Huizenga

Fusion Reactions between Heavy Nuclei

doi: 10.1146/annurev.ns.33.120183.001405
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1983BR19      Phys.Rev. C28, 1080 (1983)

H.Breuer, A.C.Mignerey, V.E.Viola, K.L.Wolf, J.R.Birkelund, D.Hilscher, J.R.Huizenga, W.U.Schroder, W.W.Wilcke

Charge and Mass Exchange in 56Fe-Induced Reactions at 8.3 MeV/Nucleon

NUCLEAR REACTIONS 56Fe, 165Ho, 209Bi, 238U(56Fe, X), E=465 MeV; measured σ(fragment Z, mass); deduced neutron, proton distribution centroids, variances, correlation coefficients, charge equilibration, reaction mechanisms. Gaussian function fits.

doi: 10.1103/PhysRevC.28.1080
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1983HU09      Phys.Rev. C28, 1853 (1983)

J.R.Huizenga, J.R.Birkelund, L.E.Tubbs, D.Hilscher, U.Jahnke, H.Rossner, B.Gebauer, H.Lettau

Limitation of Linear Momentum Transfer in Heavy-Ion Reactions

NUCLEAR REACTIONS 165Ho, 181Ta, 197Au, 209Bi, 238U(20Ne, F), E=292 MeV; measured fission fragment σ(θ1, θ2); deduced linear momentum transfer limitations. Rolling collision model.

doi: 10.1103/PhysRevC.28.1853
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1983KO34      Phys.Lett. 133B, 153 (1983)

J.P.Kosky, W.W.Wilcke, J.R.Birkelund, M.A.Butler, A.D.Dougan, J.R.Huizenga, W.U.Schroder, H.J.Wollersheim, D.Hilscher

Alpha-Particle Emission in the Strongly Damped Reaction of 156Ho + 56Fe at 8.3 MeV/Nucleon

NUCLEAR REACTIONS 165Ho(56Fe, X), E=465 MeV; measured α(fragment)-coin, α-multiplicity vs fragment Z; deduced α-emission mechanism.

doi: 10.1016/0370-2693(83)90549-X
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1983RO09      Phys.Rev. C27, 2666 (1983)

H.Rossner, D.Hilscher, E.Holub, G.Ingold, U.Jahnke, H.Orf, J.R.Huizenga, J.R.Birkelund, W.U.Schroder, W.W.Wilcke

Angular Distributions of Fragments from Fission Induced by 220-MeV 20Ne on Targets of 165Ho, 197Au, and 209Bi

NUCLEAR REACTIONS 165Ho, 197Au, 209Bi(20Ne, F), E=220 MeV; measured fission fragment σ(θ). 197Ir, 211Ac, 223Np, 175Re, 207Fr, 219Pa; deduced prefission multi-neutron induced angular momentum dealignment effect. Liquid drop, rotating liquid drop models, incomplete fusion, prefission particle emission mechanisms.

doi: 10.1103/PhysRevC.27.2666
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1983WI06      Phys.Rev.Lett. 51, 99 (1983)

W.W.Wilcke, J.P.Kosky, J.R.Birkelund, M.A.Butler, A.D.Dougan, J.R.Huizenga, W.U.Schroder, H.J.Wollersheim, D.Hilscher

New Mechanism of α-Particle Production in Heavy-Ion-Induced Fission

NUCLEAR REACTIONS 165Ho(56Fe, αF), E=465 MeV; measured fission (fragment)(fragment)α-coin, α-multiplicity vs θα, Eα; deduced α-production mechanism.

doi: 10.1103/PhysRevLett.51.99
Citations: PlumX Metrics

1982BI10      Phys.Rev. C26, 1984 (1982)

J.R.Birkelund, H.Freiesleben, J.R.Huizenga, W.U.Schroder, W.W.Wilcke, K.L.Wolf, J.P.Unik, V.E.Viola, Jr.

Mechanisms of Heavy Ion Dissipative Collisions: The 209Bi + 84Kr reaction at E(lab) = 712 MeV

NUCLEAR REACTIONS 209Bi(84Kr, X), E=712 MeV; measured σ(fragment θ, E, Z); deduced correlation variables kinetic energy dissipation dependence. Dissipative collisions, proximity one-body transport model.

doi: 10.1103/PhysRevC.26.1984
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1982HO01      Phys.Rev. C25, 256 (1982)

A.D.Hoover, J.R.Birkelund, D.Hilscher, W.U.Schroder, W.W.Wilcke, J.R.Huizenga, H.Breuer, A.C.Mignerey, V.E.Viola, Jr., K.L.Wolf

165Ho + 56Fe Reaction at E(lab) = 462 MeV

NUCLEAR REACTIONS 165Ho(56Fe, X), E=462 MeV; measured σ(fragment, θ, E, Z); deduced interaction times. Dynamical calculations.

doi: 10.1103/PhysRevC.25.256
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1982WO01      Phys.Rev. C25, 338 (1982)

H.J.Wollersheim, W.W.Wilcke, J.R.Birkelund, J.R.Huizenga

Influence of the Impact Parameter on Element Distributions in Dissipative Heavy-Ion Collisions

NUCLEAR REACTIONS 209Bi(136Xe, X), E=940, 1130, 1422 MeV; calculated fragment mean kinetic energy vs (L); deduced initial angular momentum, interaction time, charge diffusion coefficient.

doi: 10.1103/PhysRevC.25.338
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1981SC02      Phys.Lett. 98B, 355 (1981)

W.U.Schroder, J.R.Huizenga, J.Randrup

Correlated Mass and Charge Transport Induced by Statistical Nucleon Exchange in Damped Nuclear Reactions

NUCLEAR REACTIONS 165Ho, 238U, 56Fe(56Fe, X), E=464 MeV; analyzed fragment mass, charge variance distributions vs energy loss. Statistical nucleon exchange, damped collisions, transport model.

doi: 10.1016/0370-2693(81)90924-2
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1981WO06      Phys.Rev. C24, 2114 (1981)

H.J.Wollersheim, W.W.Wilcke, J.R.Birkelund, J.R.Huizenga, W.U.Schroder, H.Freiesleben, D.Hilscher

209Bi + 136Xe Reaction at E(lab) = 1422 MeV

NUCLEAR REACTIONS 209Bi(136Xe, X), E=1422 MeV; measured σ(fragment E, Z, θ); deduced reaction mechanism, element distribution first, second moments. One-body transport model.

doi: 10.1103/PhysRevC.24.2114
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1980BR26      Phys.Rev. C22, 2454 (1980)

H.Breuer, K.L.Wolf, B.G.Glagola, K.K.Kwiatkowski, A.C.Mignerey, V.E.Viola, W.W.Wilcke, W.U.Schroder, J.R.Huizenga, D.Hilscher, J.Birkelund

Production of Neutron-Excess Nuclei in 56Fe-Induced Reactions

NUCLEAR REACTIONS 238U, 209Bi(56Fe, X), E=8.3 MeV/nucleon; measured yields for 52,53Sc, 54,55,56Ti, 56,57,58V, 58,59,60Cr, 61Mn, 63Fe.

doi: 10.1103/PhysRevC.22.2454
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1980MI10      Phys.Rev.Lett. 45, 509 (1980)

A.C.Mignerey, V.E.Viola, Jr., H.Breuer, K.L.Wolf, B.G.Glagola, J.R.Birkelund, D.Hilscher, J.R.Huizenga, W.U.Schroder, W.W.Wilcke

Dependence of Isobaric Charge Distributions on Energy Loss and Mass Asymmetry in Damped Collisions

NUCLEAR REACTIONS 56Fe, 165Ho, 238U(56Fe, X), E=8.3 MeV/nucleon; measured σ(fragment E, mass, Z); deduced isobaric charge, isotopic mass distribution variances vs energy loss. Equilibration models, damped collisions.

doi: 10.1103/PhysRevLett.45.509
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1980SC02      Phys.Rev.Lett. 44, 308 (1980)

W.U.Schroder, J.R.Birkelund, J.R.Huizenga, W.W.Wilcke, J.Randrup

Effect of Pauli Blocking on Exchange and Dissipation Mechanisms Operating in Heavy-Ion Reactions

NUCLEAR REACTIONS 209Bi(136Xe, X), E=940, 1130 MeV; 209Bi(56Fe, X), E=465 MeV; calculated energy loss vs fragment Z distribution variance. Exchange-induced dissipation mechanism, Pauli principle.

doi: 10.1103/PhysRevLett.44.308
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1980VI04      Phys.Rev. C22, 122 (1980)

V.E.Viola, Jr., A.C.Mignerey, H.Breuer, K.L.Wolf, B.G.Glagola, W.W.Wilcke, W.U.Schroder, J.R.Huizenga, D.Hilscher, J.R.Birkelund

Possible Production of Actinide Spontaneous Fission Activities in Damped Collisions of 209Bi + 56Fe

RADIOACTIVITY 240,242,244Am, 234,236,238,240Cf, 242,244,246Fm [from 209Bi(56Fe, X), E=464 MeV]; measured T1/2 for SF.

NUCLEAR REACTIONS 209Bi(56Fe, X), E=464 MeV; measured σ(fragment, Z), actinide element production σ.

doi: 10.1103/PhysRevC.22.122
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0782.

1980WI06      Phys.Rev. C21, 2019 (1980)

W.W.Wilcke, M.W.Johnson, W.U.Schroder, D.Hilscher, J.R.Birkelund, J.R.Huizenga, J.C.Browne, D.G.Perry

Actinide Muonic Atom Lifetimes Deduced from Muon-Induced Fission

NUCLEAR REACTIONS 235,238U, 237Np, 239,242Pu(μ-, F), E at rest; measured delayed fission. 232Th, 233,235,238U, 237Np, 239,242Pu deduced muon capture rates, T1/2 of muonic atoms, isotopic effects.

doi: 10.1103/PhysRevC.21.2019
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1980WI08      Phys.Rev. C22, 128 (1980)

W.W.Wilcke, J.R.Birkelund, A.D.Hoover, J.R.Huizenga, W.U.Schroder, V.E.Viola, Jr., K.L.Wolf, A.C.Mignerey

Bombarding-Energy Dependence of the 209Bi + 136Xe Reaction

NUCLEAR REACTIONS 209Bi(136Xe, X), E=940 MeV; measured σ(θ, E, Z); deduced correlations, interaction times, transport coefficients, sequential fission probability. Damped reaction, trajectory calculation.

doi: 10.1103/PhysRevC.22.128
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1980WI21      At.Data Nucl.Data Tables 25, 389 (1980)

W.W.Wilcke, J.R.Birkelund, H.J.Wollersheim, A.D.Hoover, J.R.Huizenga, W.U.Schroder, L.E.Tubbs

Reaction Parameters for Heavy-Ion Collisions

COMPILATION 12C, 56Fe, 140Ce, 197Au, 16O, 27Al, 40Ca, 63Cu, 92Mo, 108Ag, 154Sm, 208Pb, 165Ho, 181Ta, 209Bi, 238U; compiled reaction parameters for different projectiles, E=1-50 MeV/nucleon. Fresnel, droplet, rotating liquid drop models, data systematics, heavy ions.

doi: 10.1016/0092-640X(80)90010-8
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1979BR13      Phys.Rev.Lett. 43, 191 (1979)

H.Breuer, B.G.Glagola, V.E.Viola, K.L.Wolf, A.C.Mignerey, J.R.Birkelund, D.Hilscher, A.D.Hoover, J.R.Huizenga, W.U.Schroder, W.W.Wilcke

Nucleon Exchange and A/Z Equilibration in Interactions of 8.3-MeV/amu 56Fe Ions with 56Fe, 165Ho, and 209Bi

NUCLEAR REACTIONS 56Fe, 165Ho, 209Bi(56Fe, X), E=8.3 MeV/nucleon; measured σ for Fe-like fragments; deduced dependence of fragment A/Z ratio, A-Z variance relationships on damping.

doi: 10.1103/PhysRevLett.43.191
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1979HI01      Phys.Rev. C20, 556 (1979)

D.Hilscher, J.R.Birkelund, A.D.Hoover, W.U.Schroder, W.W.Wilcke, J.R.Huizenga, A.C.Mignerey, K.L.Wolf, H.F.Breuer, V.E.Viola

Structure in the Energy Spectra of the Fragments Produced in Damped Heavy-Ion Reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), E=400 MeV; calculated production σ(E) for 41Ca. Statistical evaporation process for HI damped collisions.

doi: 10.1103/PhysRevC.20.556
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1979HI02      Phys.Rev. C20, 576 (1979)

D.Hilscher, J.R.Birkelund, A.D.Hoover, W.U.Schroder, W.W.Wilcke, J.R.Huizenga, A.C.Mignerey, K.L.Wolf, H.F.Breuer, V.E.Viola, Jr.

Neutron Emission in the Reaction 165Ho + 56Fe at E(lab) = 8.5 MeV/u

NUCLEAR REACTIONS 165Ho(56Fe, xn), (56Fe, α), E=476 MeV; measured σ(E, θ, φ); deduced nuclear temperatures, neutron multiplicities, N/Z, neutron out-of-plane anisotropy, reaction mechanism.

doi: 10.1103/PhysRevC.20.576
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1979SC19      Phys.Rev.Lett. 43, 672 (1979)

W.U.Schroder, W.W.Wilcke, M.W.Johnson, D.Hilscher, J.R.Huizenga, J.C.Browne, D.G.Perry

Evidence for Atomic Muon Capture by Fragments from Prompt Fission of Muonic 237Np, 239Pu, and 242Pu

NUCLEAR REACTIONS 237Np, 239,242Pu(μ-, nF), E=at rest; measured (fragment n)-coin; deduced T1/2 of muon bound to target, target-n, fission fragment.

doi: 10.1103/PhysRevLett.43.672
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1978BI05      Phys.Rev.Lett. 40, 1123 (1978)

J.R.Birkelund, J.R.Huizenga, J.N.De, D.Sperber

Heavy-Ion Fusion Based on the Proximity Potential and One-Body Friction

NUCLEAR REACTIONS 27Al(16O, X), 58,60,62,64Ni, 112,116,120,124Sn(35Cl, X), 109Ag(40Ar, X); calculated fusion σ.

doi: 10.1103/PhysRevLett.40.1123
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1978DE40      S.Afr.J.Phys. 1, 239 (1978)

J.N.De, A.Sherman, D.Sperber, J.R.Birkelund, J.R.Huizenga

Fusion-Excitation Functions as a Test of the Radial Dependence of the Proximity Potential

NUCLEAR REACTIONS 27Al(35Cl, X), E(cm)=50-300 MeV; 232Th(40Ar, X), E(cm)=20-55 MeV; calculated σ(fusion, E); deduced radial dependence of ion-ion potential. Proximity potential model.

1978GR12      Phys.Rev. C18, 671 (1978)

R.D.Griffioen, R.C.Thompson, J.R.Huizenga

Levels of 235Np Excited by the 234U(3He, d) and 234U(α, t) Reactions

NUCLEAR REACTIONS 234U(3He, d), (α, t), E=30 MeV; measured σ(θ). 235Np deduced levels, Nilsson configurations. Enriched target.

doi: 10.1103/PhysRevC.18.671
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1978JO05      Phys.Rev. C17, 927 (1978)

M.W.Johnson, R.C.Thompson, J.R.Huizenga

States in U233 Excited by the 234U(d, t) and 234U(3He, α) Reactions

NUCLEAR REACTIONS 234U(d, t), E=14 MeV; 234U(3He, α), E=30 MeV; measured σ(θ). 233U deduced levels, L, Nilsson configurations, J, π.

doi: 10.1103/PhysRevC.17.927
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1978WI07      Phys.Rev. C18, 1452 (1978)

W.W.Wilke, M.W.Johnson, W.U.Schroder, J.R.Huizenga, D.G.Perry

Neutron Emission from Actinide Muonic Atoms

NUCLEAR REACTIONS 232Th, 235,238U, 237Np, 239,242Pu(μ-, F), E=0 MeV; measured n(t); deduced total muon capture rates, isotope effect, Γn/Γf.

doi: 10.1103/PhysRevC.18.1452
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1977FE11      Phys.Lett. 69B, 407 (1977)

W.Feix, W.Wilcke, T.W.Elze, H.Rebel, J.R.Huizenga, R.C.Thompson, R.M.Dreizler

Study of Nuclear-Coulomb Interference Effects in Inelastic Deuteron Scattering on 238U

NUCLEAR REACTIONS 238U(d, d), (d, d'), E=17 MeV; measured σ(θ). 238U deduced β.

doi: 10.1016/0370-2693(77)90831-0
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1977JO09      Phys.Rev. C15, 2169 (1977)

M.W.Johnson, W.U.Schroder, J.R.Huizenga, W.K.Hensley, D.G.Perry, J.C.Browne

Measurement of Total Muon-Capture Rates in 232Th, 235,238U, and 239Pu

RADIOACTIVITY 232Th, 235,238U, 239Pu; measured muon disappearance rates in muonic atoms; deduced total muon capture rates, upper limit for population of shape isomers.

doi: 10.1103/PhysRevC.15.2169
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1977SC29      Phys.Lett. 71B, 283 (1977)

W.U.Schroder, J.R.Huizenga, J.R.Birkelund, K.L.Wolf, V.E.Viola, Jr.

Dissipation, Mass-Exchange and the Microscopic Time Scale of Heavy-Ion Collisions

NUCLEAR REACTIONS 165Ho, 209Bi(136Xe, X), 165Ho(84Kr, X), 197Au(86Kr, X); calculated energy loss/exchanged nucleon.

doi: 10.1016/0370-2693(77)90216-7
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1977TH04      Phys.Rev. C15, 2019 (1977)

R.C.Thompson, W.Wilcke, J.R.Huizenga, W.K.Hensley, D.G.Perry

Levels of Isotopes 233,235,237Pa and 229,231Ac Studied by the (t, α) Reaction

NUCLEAR REACTIONS 234,236,238U, 230,232Th(t, α), E=15 MeV; measured σ(Eα, θ). 233,235,237Pa, 229,231Ac deduced levels, J, S, Nilsson proton configurations. DWBA analysis.

doi: 10.1103/PhysRevC.15.2019
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1977WI07      Nucl.Phys. A286, 297 (1977)

W.Wilcke, W.Feix, T.W.Elze, J.R.Huizenga, R.C.Thompson, R.M.Dreizler

Influence of Form Factors and Multistep Effects on the 232Th(d, t)231Th Reaction

NUCLEAR REACTIONS 232Th(d, t), E=17 MeV; measured σ(Et, θ). 230Th(d, p), E=17 MeV; measured σ(Ep, 80°). 231Th levels deduced S.

doi: 10.1016/0375-9474(77)90409-2
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1976BI01      Phys.Rev. C13, 133 (1976)

J.R.Birkelund, J.R.Huizenga, H.Freiesleben, K.L.Wolf, J.P.Unik, V.E.Viola, Jr.

Elastic Scattering of 40Ar and 84Kr on 209Bi and 238U at 7.2 and 8.5 MeV/N

NUCLEAR REACTIONS 209Bi, 238U(40Ar, 40Ar), E=340 MeV; 209Bi(84Kr, 84Kr), E=600, 712 MeV; measured σ(θ); deduced maximum angular momenta, interaction radii, total σ. Optical, Fresnel model analysis.

doi: 10.1103/PhysRevC.13.133
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1976SC04      Phys.Rev.Lett. 36, 514 (1976)

W.U.Schroder, J.R.Birkelund, J.R.Huizenga, K.L.Wolf, J.P.Unik, V.E.Viola, Jr.

Study of the Reaction 209Bi + 136Xe

NUCLEAR REACTIONS 209Bi(136Xe, X), E=1130 MeV; measured σ(E(fragment mass), θ).

doi: 10.1103/PhysRevLett.36.514
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1976TH01      Phys.Rev. C13, 638 (1976)

R.C.Thompson, J.R.Huizenga, T.W.Elze

Collective States in 233U, 235U, 237Np, and 239Pu Excited by Inelastic Deuteron Scattering

NUCLEAR REACTIONS 233,235U, 237Np, 239Pu(d, d'), E=16 MeV; measured σ(Ed'). 233,235U, 237Np, 239Pu deduced levels, K, J, π. Enriched targets.

doi: 10.1103/PhysRevC.13.638
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1975BO08      Phys.Rev. C11, 1265 (1975)

J.P.Bondorf, J.R.Huizenga, M.I.Sobel, D.Sperber

Classical Model for Strongly Damped Collisions in Heavy-Ion Reactions

NUCLEAR REACTIONS 209Bi(84Kr, X), E=600 MeV; analyzed reaction.

doi: 10.1103/PhysRevC.11.1265
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1975EL03      Z.Phys. A272, 119 (1975)

T.W.Elze, J.R.Huizenga

Levels of 233Pa Excited in Helium-Induced Single-Proton Transfer Reactions

NUCLEAR REACTIONS 232Th(3He, d), E=28.5 MeV; measured σ(Ed, θ). 232Th(α, t), E=30 MeV; measured σ(Et, θ). 233Pa deduced levels, K, J, π, L.

doi: 10.1007/BF01408436
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1975FR12      Phys.Rev. C12, 42 (1975)

H.Freiesleben, G.T.Rizzo, J.R.Huizenga

6Li and 7Li Induced Fission of 232Th and 238U

NUCLEAR REACTIONS 232Th, 238U(6Li, 6Li), (7Li, 7Li), E=37.2 MeV; measured σ(θ). 232Th, 238U(6Li, F), (7Li, F), E=24-38.4 MeV; measured total σ(θ).

doi: 10.1103/PhysRevC.12.42
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1975HU07      Nukleonika 20, 291 (1975)


Selected Aspects of Very Heavy Ion Reactions

NUCLEAR REACTIONS 109Ag, 165Ho, 197Au, 209Bi, 232Th, 238U, 121Sb(40Ar, X), 186W(63Cu, X), 165Ho, 181Ta, 186W, 197Au, 208Pb, 209Bi(84Kr, X), 133Cs(136Xe, X); calculated nothing, discussed reactions.

1975TH04      Nucl.Phys. A242, 1 (1975)

R.C.Thompson, J.S.Boyno, J.R.Huizenga, D.G.Burke, T.W.Elze

Study of the 188Os(p, t)186Os, 190Os(p, t)188Os and 192Os(p, t)190Os Reactions

NUCLEAR REACTIONS 188,190,192Os(p, t), E=18 MeV; measured σ(Et, θ); deduced Q. 186,188,190Os deduced levels, J, π, L. 189Os(p, t), E=18 MeV; calculated Q.

doi: 10.1016/0375-9474(75)90029-9
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1975TH11      Phys.Rev. C12, 1227 (1975)

R.C.Thompson, J.R.Huizenga, T.W.Elze

Collective States in 230Th, 240Pu, 244Pu, and 248Cm Excited by Inelastic Deuteron Scattering

NUCLEAR REACTIONS 230Th, 240,244Pu, 248Cm(d, d'), E=16 MeV; measured σ(Ed', θ). 230Th, 240,244Pu, 248Cm deduced levels, J, K, π, B(E2), B(E3). Enriched targets.

doi: 10.1103/PhysRevC.12.1227
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1975VO01      Phys.Rev. C11, 529 (1975)

T.von Egidy, T.W.Elze, J.R.Huizenga

Nuclear Levels of 239Np Excited by the (3He, d) and (α, t) Reactions

NUCLEAR REACTIONS 238U(3He, d), (α, t), E=28.5 MeV; measured σ(Ed, θ), σ(Et, θ). 239Np deduced levels, J, π, K.

doi: 10.1103/PhysRevC.11.529
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1521.

1974BR03      Phys.Rev. C9, 435 (1974)

H.C.Britt, J.R.Huizenga

Reevaluation of Experimental Estimates of the Pairing Gap at the Fission Saddle Point

NUCLEAR STRUCTURE 236U, 240Pu; reevaluate pairing gap at fission saddle point.

doi: 10.1103/PhysRevC.9.435
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1974FR05      Nucl.Phys. A224, 503 (1974)

H.Freiesleben, J.R.Huizenga

Total Reaction Cross Sections of Deformed Nuclei: A Study of the 233,238U + α Systems

NUCLEAR REACTIONS 233,238U(α, α), (α, F), Eα=15-27 MeV; measured σ(scatt)(Eα, θ), σ(fission)(Eα). Total reaction cross sections, interaction barrier deduced. Enriched targets.

doi: 10.1016/0375-9474(74)90552-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2486.

1974FR07      Phys.Rev. C10, 245 (1974)

H.Freiesleben, H.C.Britt, J.Birkelund, J.R.Huizenga

6Li, 7Li Induced Reactions on 209Bi

NUCLEAR REACTIONS 209Bi(6Li, xn), (7Li, xn), (6Li, F), (7Li, F), (7Li, xnα), (7Li, xnt), 209Bi(7Li, αp), (6Li, xnd), (6Li, α), E=25-34 MeV; measured σ(E).

doi: 10.1103/PhysRevC.10.245
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1974HU07      Nucl.Phys. A223, 577 (1974)

J.R.Huizenga, A.N.Behkami, J.S.Sventek, R.W.Atcher

Comparison of Neutron Resonance Spacings with Microscopic Theory for Spherical Nuclei

COMPILATION A=20-148; A=181-209; compiled level spacings.

doi: 10.1016/0375-9474(74)90707-6
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1974HU08      Nucl.Phys. A223, 589 (1974)

J.R.Huizenga, A.N.Behkami, R.W.Atcher, J.S.Sventek, H.C.Britt, H.Freiesleben

Comparison of Neutron Resonance Spacings with Microscopic Theory for Nuclei with Static Deformation

COMPILATION A=150-248; compiled level spacings.

doi: 10.1016/0375-9474(74)90708-8
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1974KA10      Nucl.Phys. A222, 405 (1974)

C.Kalbach-Cline, J.R.Huizenga, H.K.Vonach

Isospin Conservation and Pre-Equilibrium Decay in (p, p') Reactions on Neutron Rich Tin Isotopes

NUCLEAR REACTIONS 112,118,120,124Sn(p, p'), E=14.0, 17.8 MeV; measured σ(Ep', θ); enriched targets.

doi: 10.1016/0375-9474(74)90400-X
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1974WO07      Phys.Rev.Lett. 33, 1105 (1974)

K.L.Wolf, J.P.Unik, J.R.Huizenga, J.Birkelund, H.Freiesleben, V.E.Viola

Study of Strongly Damped Collisions in the Reaction of 600-MeV 84Kr on A 209Bi Target

NUCLEAR REACTIONS 209Bi(84Kr, X), E=600 MeV; measured σ(fragment mass); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.33.1105
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1973BE57      Nucl.Phys. A217, 78 (1973)

A.N.Behkami, J.R.Huizenga

Comparison of Experimental Level Densities and Spin Cutoff Factors with Microscopic Theory for Nuclei Near A = 60

NUCLEAR STRUCTURE 55Mn, 56Fe, 59Co, 60,62Ni, 63,65Cu; calculated level density, spin cutoff factor.

doi: 10.1016/0375-9474(73)90624-6
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1973BO27      Nucl.Phys. A209, 125 (1973)

J.S.Boyno, J.R.Huizenga, T.W.Elze, C.E.Bemis, Jr.

Levels of 234U and 236U Excited by the (d, d') Reaction

NUCLEAR REACTIONS 234,236U(d, d'), E=16 MeV; measured σ(Ed', θ=90°, 125°). 234,236U deduced levels, J, π, B(E2), B(E3). Enriched targets.

doi: 10.1016/0375-9474(73)90056-0
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1973HE27      Science 181, 1164 (1973)

W.K.Hensley, W.A.Bassett, J.R.Huizenga

Pressure Dependence of the Radioactive Decay Constant of Beryllium-7

NUCLEAR STRUCTURE 7Be; calculated decay constant.

doi: 10.1126/science.181.4105.1164
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1973KI10      Phys.Rev. C8, 1965 (1973)

M.Kildir, J.R.Huizenga

Isospin Dependence of the Nuclear Level Width

NUCLEAR REACTIONS 31P(p, α), (p, p'), E=8.5-10.0 MeV, measured σ(E;θ). 32S deduced level widths, level densities for isospin states at 17.8 MeV.

doi: 10.1103/PhysRevC.8.1965
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0769.

1972BO47      Phys.Rev. C6, 1411 (1972)

J.S.Boyno, J.R.Huizenga

Levels of 155,157,159,161Tb Excited in Helium-Induced Single-Proton-Transfer Reactions

NUCLEAR REACTIONS 154,156,158,160Gd(3He, d), (α, t), E=25.5 MeV, Eα=27 MeV; measured σ(θ). 155,157,159,161Tb deduced levels, S, L(p), Nilsson assignments.

doi: 10.1103/PhysRevC.6.1411
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1972EL07      Nucl.Phys. A187, 473 (1972)

T.W.Elze, J.S.Boyno, J.R.Huizenga

Collective States of Gd Isotopes from (p, t) Reactions

NUCLEAR REACTIONS 160,158,156,154,152Gd(p, t), E=18 MeV; measured σ(Et, θ). 158,156,154,152,150Gd deduced levels, L, J, π. Isotope-separated targets.

doi: 10.1016/0375-9474(72)90672-0
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1972EL08      Nucl.Phys. A187, 545 (1972)

T.W.Elze, J.R.Huizenga

Collective States of 232Th, 238U and 242Pu

NUCLEAR REACTIONS 232Th, 238U, 242Pu(d, d'), Ed=16 MeV; measured σ(Ed', θ=90°, 125°); 232Th(d, d), Ed=16 MeV; measured σ(θ). 232Th, 238U, 242Pu deduced levels, J, π, B(E2), B(E3). Enriched targets.

doi: 10.1016/0375-9474(72)90679-3
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1972LU03      Nucl.Phys. A190, 229 (1972)

C.C.Lu, L.C.Vaz, J.R.Huizenga

Level Densities from Spectra of Different Reactions Populating the Same Nucleus

NUCLEAR REACTIONS 59Co, 62Ni, 63,65Cu(p, p'), (p, α), E approx 12 MeV; 56Fe, 59Co, 60,62Ni(α, p), (α, α'), E approx 16 MeV; 63,65Cu(α, α'), E=17 MeV; measured, calculated σ(Eα'), σ(Eα), σ(Ep'), σ(Ep). 56Fe, 59Co, 60Ni, 62Ni, 63Cu, 65Cu deduced level density parameters. Isotopically separated targets.

doi: 10.1016/0375-9474(72)90139-X
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1972LU09      Nucl.Phys. A197, 321 (1972)

C.C.Lu, L.C.Vaz, J.R.Huizenga

Spin Distribution of the Nuclear Level Density Near A = 60

NUCLEAR REACTIONS 56Fe(α, α'), 59Co(α, α'), 60Ni(α, α'), 62Ni(α, α'), 63Cu(α, α'), E=17.0 MeV; 60Ni(α, p), , 62Ni(α, p), E=16.5, 16.2 MeV; measured σ(Eα', θ), σ(Ep, θ). 56Fe, 59Co, 60,62Ni, 63,65Cu deduced spin cut-off factors. Isotopically separated targets.

doi: 10.1016/0375-9474(72)91014-7
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1972VA03      Phys.Rev. C5, 463 (1972)

L.C.Vaz, C.C.Lu, J.R.Huizenga

Isospin and the Bohr Independence Hypothesis

NUCLEAR REACTIONS 63Cu(p, p'), (p, α), E=12 MeV; 60Ni(α, α'), (α, p), E=16.6 MeV; measured σ(Ep'), σ(Eα), σ(Eα'), σ(Ep), σ ratios.

doi: 10.1103/PhysRevC.5.463
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2677.

1972VA31      Phys.Rev. C6, 1896 (1972)

L.C.Vaz, C.C.Lu, J.R.Huizenga

Level Densities from Analysis of Particle Spectra

doi: 10.1103/PhysRevC.6.1896
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1972WI13      Nucl.Phys. A187, 225 (1972)

F.C.Williams, Jr., G.Chan, J.R.Huizenga

The Significance of Shell Corrections in the Parameterization of Numerical State Density Calculations

NUCLEAR STRUCTURE A=20-242, Z=9-94; analyzed significance of shell corrections in parameterization of state density calculations.

doi: 10.1016/0375-9474(72)90576-3
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1971EL02      Phys.Rev. C3, 234 (1971)

T.W.Elze, J.R.Huizenga

Study of the 242Pu(d, t)241Pu and 242Pu(3He, α)241Pu Reactions

NUCLEAR REACTIONS 242Pu(d, t), E=17 MeV; 242Pu(3He, α), E=30 MeV; measured σ(Et, θ), σ(Eα, θ). 241Pu deduced levels, J, π, L(n), S.

doi: 10.1103/PhysRevC.3.234
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1971LU03      Nucl.Phys. A164, 225 (1971)

C.C.Lu, J.R.Huizenga, C.J.Stephan, A.J.Gorski

Effects of Isospin on Statistical Nuclear Decay

NUCLEAR REACTIONS 59Co, 62Ni(p, p'), (p, α), E=13 MeV; measured σ(Ep'), σ(Eα); 59Co(α, p), (α, α')E=14.1 MeV; measured σ(Ep), σ(Eα'); 56Fe(α, p), (α, α'), E=17.2 MeV; measured σ(Ep), σ(Eα'); deduced violation of Bohr-independence hypothesis by isospin selection rule. Enriched targets.

doi: 10.1016/0375-9474(71)90210-7
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1971YU01      Nucl.Phys. A171, 614 (1971)

G.Yuen, G.T.Rizzo, A.N.Behkami, J.R.Huizenga

Fragment Angular Distributions of the Neutron-Induced Fission of 230Th

NUCLEAR REACTIONS, Fission 230Th(n, F), En=682, 715, 730, 740(5 keV energy resolution), En=750, 1000(20 keV energy resolution); measured σ(En, θ(fragment)). 231Th deduced vibrational-mode resonance state with K=1/2.

doi: 10.1016/0375-9474(71)90607-5
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1970BO31      Nucl.Phys. A157, 263 (1970)

J.S.Boyno, T.W.Elze, J.R.Huizenga

A Study of the 232Th(d, t)231Th and 238U(d, t)237U Reactions

NUCLEAR REACTIONS 232Th(d, t), 238U(d, t), E=17 MeV; measured σ(Et, 60°). 231Th, 237U deduced levels, J, π, L, K, S. Natural targets.

doi: 10.1016/0375-9474(70)90112-0
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1970EL02      Phys.Rev. C1, 328 (1970)

T.W.Elze, J.R.Huizenga

Levels of 237Np Excited by the 236U(3He, d)237Np and 236U(α, t)237Np Reactions

NUCLEAR REACTIONS 236U(3He, d), (α, t), E=30 MeV; measured σ(Ed), σ(Et). 237Np deduced levels, S, rotational band assignments.

doi: 10.1103/PhysRevC.1.328
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1970EL07      Nucl.Phys. A149, 585 (1970)

T.W.Elze, J.R.Huizenga

Energy Levels of 243Am Excited by the 242Pu(3He, d) and 242Pu(α, t) Reactions

NUCLEAR REACTIONS 242Pu(3He, d), 242Pu(α, t), E=30 MeV; measured σ(Ed, θ=60°), σ(Et, θ=45°). 243Am deduced levels, J, K, π, L, S. Enriched target.

doi: 10.1016/0375-9474(70)91049-3
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1970OT02      Nucl.Phys. A144, 502 (1970)

K.Otozai, J.W.Meadows, A.N.Behkami, J.R.Huizenga

Fragment Angular Distributions from Neutron-Induced Fission of 242Pu

NUCLEAR REACTIONS, Fission 242Pu(n, F), En=500, 620, 730, 990, 1230 keV; measured σ(En, θ(fragment)). 243Pu deduced information on transition states.

doi: 10.1016/0375-9474(70)90341-6
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1970VO03      Nucl.Phys. A145, 306 (1970)

T.von Egidy, T.W.Elze, J.R.Huizenga

Nuclear Levels of 237U Excited by the (3He, α) Reaction

NUCLEAR REACTIONS 238U(3He, α), E=30 MeV; measured σ(Eα, θ). 237U deduced levels, J, π, L, K, S. Natural target.

doi: 10.1016/0375-9474(70)90321-0
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1969EL03      Nucl.Phys. A128, 564 (1969)

T.W.Elze, T.v.Egidy, J.R.Huizenga

A Study of the 232Th(3He, α)231Th Reaction

NUCLEAR REACTIONS 232Th(3He, α), E=30 MeV; measured σ(Eα, θ). 231Th deduced levels, J, π, L, S. Natural target.

doi: 10.1016/0375-9474(69)90423-0
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1969EL04      Nucl.Phys. A133, 10 (1969)

T.W.Elze, J.R.Huizenga

A Study of the 236U(3He, α)235U Reaction

NUCLEAR REACTIONS 236U(3He, α), E=30 MeV; measured σ(Eα, θ). 235U deduced levels, J, π, L, S. Enriched target.

doi: 10.1016/0375-9474(69)90445-X
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1969HU11      Phys.Rev. 182, 1149 (1969)

J.R.Huizenga, H.K.Vonach, A.A.Katsanos, A.J.Gorski, C.J.Stephan

Level Densities from Excitation Functions of Isolated Levels

NUCLEAR REACTIONS 56Fe(α, p), E = 12-19 MeV; 55Mn, 59Co, 62Ni(p, α), E = 6-13.5 MeV; measured σ(E;θ). 56Fe, 60Ni, 63Cu deduced level density, spin cut-off parameter. 52Cr, 56Fe, 59Co deduced level density, spin cut-off parameters, level-width.

doi: 10.1103/PhysRev.182.1149
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1968BE59      Phys.Rev. 171, 1267 (1968)

A.N.Behkami, J.H.Roberts, W.Loveland, J.R.Huizenga

Structure of the Fission Transition Nucleus U235

NUCLEAR REACTIONS 234U(n, F), E=0.20-1.184 MeV; measured σ(θ(fragment)). 235U deduced resonances, π, K. Hauser-Feshbach analysis.

doi: 10.1103/PhysRev.171.1267
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1968BE76      Nucl.Phys. A118, 65 (1968)

A.N.Behkami, J.R.Huizenga, J.H.Roberts

Angular Distributions And Cross Sections Of Fragments From Neutron-Induced Fission Of 232Th

NUCLEAR REACTIONS 232Th(n, f), E=1.2-1.6 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12289.

doi: 10.1016/0375-9474(68)90187-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12289.

1968EL04      Phys.Letters 27B, 78 (1968)

T.W.Elze, T.Von Egidy, J.R.Huizenga

(3He, α) Reactions on Actinide Elements

NUCLEAR STRUCTURE 237U; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90163-9
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1968HU16      Phys.Rev. 174, 1539 (1968)

J.R.Huizenga, A.N.Behkami, J.W.Meadows, Jr., E.D.Klema

Nuclear Pairing Energy of Transition Nucleus Pu240

NUCLEAR REACTIONS, Fission 239Pu(n, F), E=0.15-1.5 MeV; measured σ(E;θ(fragment)). 240Pu deduced transition state, pairing energy gap.

doi: 10.1103/PhysRev.174.1539
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1968VO04      Nucl.Phys. A122, 465(1968)

H.K.Vonach, A.A.Katsanos, J.R.Huizenga

Determination of the Level Width and Density of 32S Between 17 and 21 MeV Excitation Energy

NUCLEAR REACTIONS 31P(p, α), E=8.4-11.8 MeV; measured σ(E). 32S deduced resonances, level-width.

doi: 10.1016/0375-9474(68)90055-9
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1967KA11      Phys.Rev. 159, 931 (1967)

A.A.Katsanos, J.R.Huizenga

Nuclear Energy Levels of Cr52, Mn55, and Zn66

NUCLEAR STRUCTURE 55Mn, 52Cr, 66Zn; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.159.931
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