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NSR database version of April 27, 2024.

Search: Author = W.W.Wilcke

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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
Citations: PlumX Metrics


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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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
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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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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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