NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.R.Huizenga Found 152 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1984BI06 Phys.Rev. C30, 401 (1984) 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
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
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
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
1983BI13 Ann.Rev.Nucl.Part.Sci. 33, 265 (1983) Fusion Reactions between Heavy Nuclei
doi: 10.1146/annurev.ns.33.120183.001405
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1975EL03 Z.Phys. A272, 119 (1975) 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
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
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
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
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
1974BR03 Phys.Rev. C9, 435 (1974) 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
1974FR05 Nucl.Phys. A224, 503 (1974) 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
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
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
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
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
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
1973BE57 Nucl.Phys. A217, 78 (1973) 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
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
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
1973KI10 Phys.Rev. C8, 1965 (1973) 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
1972BO47 Phys.Rev. C6, 1411 (1972) 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
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
1972EL08 Nucl.Phys. A187, 545 (1972) 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
1972LU03 Nucl.Phys. A190, 229 (1972) 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
1972LU09 Nucl.Phys. A197, 321 (1972) 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
1972VA03 Phys.Rev. C5, 463 (1972) 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
1972VA31 Phys.Rev. C6, 1896 (1972) Level Densities from Analysis of Particle Spectra
doi: 10.1103/PhysRevC.6.1896
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
1971EL02 Phys.Rev. C3, 234 (1971) 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
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
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
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
1970EL02 Phys.Rev. C1, 328 (1970) 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
1970EL07 Nucl.Phys. A149, 585 (1970) 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
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
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
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
1969EL04 Nucl.Phys. A133, 10 (1969) 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
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
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
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
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
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
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
1967KA11 Phys.Rev. 159, 931 (1967) 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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