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NSR database version of April 11, 2024.

Search: Author = R.Vandenbosch

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2000CA48      Phys.Rev. C62, 054612 (2000)

A.L.Caraley, B.P.Henry, J.P.Lestone, R.Vandenbosch

Investigation of the Level Density Parameter using Evaporative α-Particle Spectra from the 19F + 181Ta Reaction

NUCLEAR REACTIONS 181Ta(19F, X), E=121, 154, 179, 195 MeV; measured evaporation residue and fission fragment angular distributions, Ep, Eα, (evaporation residue)p-, (evaporation residue)α-coin; deduced level density parameter excitation energy dependence. Comparisons with model predictions.

doi: 10.1103/PhysRevC.62.054612
Citations: PlumX Metrics

1999KA14      Phys.Rev. C59, 2580 (1999)

S.Kailas, D.M.Nadkarni, A.Chatterjee, A.Saxena, S.S.Kapoor, R.Vandenbosch, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, J.D.Bierman

Fission Fragment Folding Angle Distributions for the Systems 11B + 237Np, 12C + 236U, and 16O + 232Th in the Energy Range 1.1 < E/VB < 2.1

NUCLEAR REACTIONS 232Th(16O, F), E=100-144.8 MeV; 236U(12C, F), E=80-130 MeV; 237Np(11B, F), E=60-118 MeV; measured fission σ, folding angle distributions; deduced momentum transfer components, fission anisotropies. Saddle-point statistical model.

doi: 10.1103/PhysRevC.59.2580
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6138.

1998LE36      Phys.Rev.Lett. 81, 4776 (1998)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Comment on ' Anomalous Peaklike Structure in the Fission Fragment Anisotropies at Sub-Barrier Energies in 11B, 12C, 16O, 19F + 232Th Reactions '

NUCLEAR REACTIONS 232Th(11B, X), E(cm)=46-66 MeV; measured fission fragments angular distributions; deduced reaction mechanism features, no peaklike structure in anisotropies.

doi: 10.1103/PhysRevLett.81.4776
Citations: PlumX Metrics

1998PR01      Phys.Rev. C57, 1305 (1998)

D.Prindle, A.Elmaani, C.Hyde-Wright, W.Jiang, A.A.Sonzogni, R.Vandenbosch, D.Bowman, G.Cron, P.Danielewicz, J.Dinius, W.Hsi, W.G.Lynch, C.Montoya, G.Peaslee, C.Schwarz, M.B.Tsang, C.Williams, R.T.de Souza, D.Fox, T.Moore

Impact Parameter Dependence of Light Charged Particle Production in 25A MeV 16O on Tb, Ta, and Au and 35A MeV 14N on Sm and Ta

NUCLEAR REACTIONS 159Tb, 181Ta, 197Au(16O, X), E=25 MeV/nucleon; 154Sm, 181Ta(14N, X), E=35 MeV/nucleon; measured p-, d-, t-, α-spectra, multiplicities, σ(θ) vs impact parameter; deduced reaction mechanism features. Transport model calculations.

doi: 10.1103/PhysRevC.57.1305
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1998SO01      Phys.Rev. C57, 722 (1998)

A.A.Sonzogni, J.D.Bierman, M.P.Kelly, J.P.Lestone, J.F.Liang, R.Vandenbosch

Transfer and Surface Vibration Couplings in the Fusion of 40Ca + 46,48,50Ti at Near-Barrier Energies

NUCLEAR REACTIONS 46,48,50Ti(40Ca, X), E=97-150 MeV; measured fusion, quasielastic σ(E, θ); deduced fusion, quasielastic σ(E), barrier distributions, surface vibration coupling parameters. Coupled-channel calculations.

doi: 10.1103/PhysRevC.57.722
Citations: PlumX Metrics

1998SO22      Phys.Rev. C58, R1873 (1998)

A.A.Sonzogni, R.Vandenbosch, A.L.Caraley, J.P.Lestone

Is Quasifission Responsible for Anomalous Fission Fragment Anisotropies ?

NUCLEAR REACTIONS 236U(12C, 4n), E=62-73 MeV; measured excitation function; deduced no quasifission competition.

doi: 10.1103/PhysRevC.58.R1873
Citations: PlumX Metrics

1997LE30      J.Phys.(London) G23, 1349 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Near- and Sub-Barrier Fission Fragment Anisotropies and the Failure ofthe Statistical Theory of Fission Decay Rates

NUCLEAR REACTIONS 232Th(16O, F), (19F, F), E(cm)=70-110 MeV; 238U(16O, F), E(cm)=75-90 MeV; 236,238U, 237Np, 232Th(12C, F), E(cm)=55-80 MeV; 232Th, 238U(11B, F), E(cm)=40-50 MeV; 238U(7Li, F), E(cm)=24-40 MeV; measured fission fragment σ(θ); deduced anisotropy, entrance channel effects, compound nucleus features. Statistical model analysis.

doi: 10.1088/0954-3899/23/10/024
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1997LE31      Phys.Rev. C56, R2907 (1997)

J.P.Lestone, A.A.Sonzogni, M.P.Kelly, R.Vandenbosch

Influence of the Ground State Spin of Target Nuclei on the Anomalous Behavior of Fission Fragment Anisotropies

NUCLEAR REACTIONS 235,236,238U(12C, F), E(cm)=57-82 MeV; measured fission σ, fragment σ(θ); deduced K-states equilibration time, anomalous behaviour target spin dependence.

doi: 10.1103/PhysRevC.56.R2907
Citations: PlumX Metrics

1997LI07      Phys.Rev.Lett. 78, 3074 (1997)

J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen

Entrance Channel Dependent Light Charged Particle Emission from the 156Er Compound Nucleus

NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 96Zr(60Ni, X), E=333 MeV; measured light charged particle energy spectra, (particle)(evaporation residue)-coin. 156Er deduced decay entrance channel dependent features.

doi: 10.1103/PhysRevLett.78.3074
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1997LI17      Phys.Rev. C56, 908 (1997)

J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen

Dissipative Effects in the Formation of the 156Er Compound Nucleus

NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 121Sb(35Cl, X), E=218 MeV; 96Zr(60Ni, X), E=333 MeV; measured E(p), I(p), E(alpha), I(alpha), (light charged particle)(residual nucleus)-coin, compound nucleus formation time scale. 156Er deduced entrance channel dependent features. Statistical model, preequilibrium decay.

doi: 10.1103/PhysRevC.56.908
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1455.

1997VA20      J.Phys.(London) G23, 1303 (1997)

R.Vandenbosch, A.A.Sonzogni, J.D.Bierman

Effects of Shape and Transfer Degrees of Freedom on Sub-Barrier Fusion

NUCLEAR REACTIONS, ICPND 194Pt(40Ca, X), E(cm)=160-200 MeV; 192Os(40Ca, X), E(cm) ≈ 150-190 MeV; measured fusion σ; 46,48,50Ti(40Ca, X), E(cm) ≈ 50-70 MeV; measured fusion σ, evaporation residue σ(θ); deduced fusion barrier distributions, shape, transfer degree of freedom effects. Coupled-channel calculations, deduced fusion barrier distributions.

doi: 10.1088/0954-3899/23/10/019
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1996BI10      Phys.Rev.Lett. 76, 1587 (1996)

J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch

Experimental Fusion Barrier Distributions Reflecting Projectile Octupole State Coupling to Prolate and Oblate Target Nuclei

NUCLEAR REACTIONS, ICPND 194Pt(40Ca, X), E(cm) ≈ 160-200 MeV; 192Os(40Ca, X), E(cm) ≈ 150-190 MeV; measured fusion σ(E); deduced targets, projectile deformations role.

doi: 10.1103/PhysRevLett.76.1587
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1996BI20      Phys.Rev. C54, 3068 (1996)

J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch

Fusion Barrier Distributions for Heavy Ion Systems Involving Prolate and Oblate Target Nuclei

NUCLEAR REACTIONS, ICPND 192Os, 194Pt(40Ca, X), E(cm)=160-200 MeV; measured fusion σ(E). 197Au(40Ca, F), E=311, 233 MeV; measured fission fragment σ(θ); deduced fusion barriers.

doi: 10.1103/PhysRevC.54.3068
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1996LO06      Nucl.Phys. A604, 219 (1996)

Y.Lou, R.T.de Souza, S.L.Chen, E.W.Cornell, B.Davin, D.Fox, T.M.Hamilton, K.Mcdonald, M.B.Tsang, T.Glasmacher, J.Dinius, C.K.Gelbke, D.O.Handzy, W.C.Hsi, M.Huang, W.G.Lynch, C.Montoya, C.Schwarz, D.Prindle, A.A.Sonzogni, R.Vandenbosch, J.L.Wile, M.Parker, D.L.Coffing

Fragment Emission from Modestly Excited Nuclear Systems

NUCLEAR REACTIONS 197Au(14N, X), E=100-156 MeV/nucleon; measured (fragment)(fragment) correlations, emission patterns; deduced emission time scale. Statistical decay model.

doi: 10.1016/0375-9474(96)00106-6
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1996SO01      Phys.Rev. C53, 243 (1996)

A.A.Sonzogni, A.Elmaani, C.Hyde-Wright, W.Jiang, D.Prindle, R.Vandenbosch, J.Dinius, G.Cron, D.Bowman, C.K.Gelbke, W.Hsi, W.G.Lynch, C.Montoya, G.Peaslee, C.Schwarz, M.B.Tsang, C.Williams, R.DeSouza, D.Fox, T.Moore

Evaporation Residue, Fission Cross Sections, and Linear Momentum Transfer for 14N Induced Reactions from 35A to 155A MeV

NUCLEAR REACTIONS 154Sm, 197Au(14N, X), (14N, F), E=35-155 MeV/nucleon; 159Tb(14N, X), (14N, F), E=35-100 MeV/nucleon; measured σ(evaporation residue θ), fission fragment σ(θ); deduced fusion σ(E). 181Ta(16O, F), E=25 MeV/nucleon; 181Ta(14N, F), E=35-100 MeV/nucleon; measured fission fragment folding angle distributions; deduced preequilibrium particle emission role.

doi: 10.1103/PhysRevC.53.243
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1996VA12      Phys.Rev. C54, R977 (1996)

R.Vandenbosch, J.D.Bierman, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, S.Kailas, D.M.Nadkarni, S.S.Kapoor

Disappearance of Entrance Channel Dependence of Fission Fragment Anisotropies at Well-Above-Barrier Energies

NUCLEAR REACTIONS 237Np(11B, F), E=60-118 MeV; 236U(12C, F), E=80-130 MeV; 232Th(16O, F), E=100-145 MeV; measured fission fragment σ(θ), anisotropies; deduced entrance channel independence.

doi: 10.1103/PhysRevC.54.R977
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6138.

1995CH05      Phys.Rev. C51, 623 (1995)

A.Charlop, J.Bierman, Z.Drebi, S.Gil, A.Sonzogni, R.Vandenbosch, D.Ye

Fusion-Fission Cross Sections for 32S + 138Ba and 48Ti + 122Sn at Near-Barrier Energies

NUCLEAR REACTIONS 138Ba(32S, F), E=150-164.7 MeV; 122Sn(48Ti, F), E=192.8-200 MeV; measured fission σ; deduced fusion σ(E). Other reactions, data analysis included. Coupled-channels model.

doi: 10.1103/PhysRevC.51.623
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1995CH06      Phys.Rev. C51, 628 (1995)

A.Charlop, J.Bierman, Z.Drebi, A.Garcia, S.Gil, D.Prindle, A.Sonzogni, R.Vandenbosch, D.Ye

Search for Entrance Channel Effects in Sub-Barrier Fusion Reactions

NUCLEAR REACTIONS 142Ce(28Si, xn), E=110-145.3 MeV; 138Ba(32S, xn), E=121.5-164.9 MeV; 122Sn(48Ti, xn), E=168.9-223.1 MeV; measured γ multiplicity; deduced < l >, no entrance channel mass asymmetry related effects. Coupled-channel model.

doi: 10.1103/PhysRevC.51.628
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1995GI02      Phys.Rev. C51, 1336 (1995)

S.Gil, F.Hasenbalg, J.E.Testoni, D.Abriola, M.C.Berisso, M.di Tada, A.Etchegoyen, J.O.Fernandez Niello, A.J.Pacheco, A.Charlop, A.A.Sonzogni, R.Vandenbosch

Fusion Cross Sections in Systems Leading to 170Hf at Near-Barrier Energies

NUCLEAR REACTIONS, ICPND 142Ce(28Si, X), E=105-145 MeV; 138Ba(32S, X), E=122-165 MeV; 122Sn(48Ti, X), E=169-222 MeV; measured E X-ray, I X-ray following fragment decay; deduced evaporation residue σ, fusion σ(E), barrier parameters.

doi: 10.1103/PhysRevC.51.1336
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1994CH06      Phys.Rev. C49, R1235 (1994)

A.Charlop, J.Bierman, Z.Drebi, A.Garcia, D.Prindle, A.A.Sonzogni, R.Vandenbosch, D.Ye, S.Gil, F.Hasenbalg, J.E.Testoni, D.Abriola, M.di Tada, A.Etchegoyen, M.C.Berisso, J.O.Fernandez-Niello, A.J.Pacheco

Absence of Anomalous Entrance Channel Effects in Sub-Barrier Heavy Ion Fusion

NUCLEAR REACTIONS 142Ce(28Si, X), 138Ba(32S, X), 122Sn(48Ti, X), E not given; measured fusion σ(E), γ multiplicity; deduced mean angular momentum. Coupled channels analysis.

doi: 10.1103/PhysRevC.49.R1235
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1994VA27      Phys.Rev. C50, 2618 (1994)


Origin of Empirical Threshold for Disspiative Fission

doi: 10.1103/PhysRevC.50.2618
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1993BI12      Phys.Rev. C48, 319 (1993)

J.D.Bierman, A.W.Charlop, D.J.Prindle, R.Vandenbosch, D.Ye

Rotational State Populations in 16O + 154Sm Near-Barrier Fusion

NUCLEAR REACTIONS 154Sm(16O, X), E=63-68 MeV; 166Er(α, X), E=43, 47.6 MeV; measured Eγ, Iγ, γγ-coin; deduced mean compound nuclear angular momenta, 4n evaporation channel.

doi: 10.1103/PhysRevC.48.319
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1993LU01      Phys.Rev. C47, 1211 (1993)

S.J.Luke, R.Vandenbosch, W.Benenson, J.Clayton, K.Joh, D.Krofcheck, T.K.Murakami, J.D.Stevenson

High Energy γ Rays from 14N + (nat)Ag at 35 MeV/nucleon

NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(θ, Eγ), high energy γ(θ). Nucleon exchange transport model, diffuse momentum distribution.

doi: 10.1103/PhysRevC.47.1211
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1993LU03      Phys.Rev. C48, 857 (1993)

S.J.Luke, R.Vandenbosch, J.Randrup

Refinements of the Nucleon-Exchange Transport Model for the Emission of Hard Photons and Nucleons

NUCLEAR REACTIONS 238U(16O, xp), E=315 MeV; Ag(16O, xp), E=30 MeV/nucleon; Ag(32S, xp), E=30 MeV/nucleon; Ta(16O, xp), E=13.5 MeV/nucleon; calculated σ(Ep, θp). Ag(14N, X), E=35 MeV/nucleon; 12C(40Ar, X), E=13 MeV/nucleon; calculated preequilibrium particle multiplicity, residue velocity. 197Au(p, X), E=34, 72 MeV; Pb(p, X), E=104 MeV; calculated σ(θγ, Eγ), hard photons. Nucleon exchange transport model, hard photon emission.

doi: 10.1103/PhysRevC.48.857
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1993PR02      Phys.Rev. C48, 291 (1993)

D.Prindle, R.Vandenbosch, S.Kailas, A.Charlop, C.Hyde-Wright

Impact Parameter Dependence of Preequilibrium Particle Emission

NUCLEAR REACTIONS 159Tb, 181Ta, Ir, 197Au(16O, F), (16O, X), E=215 MeV; measured fission (fragment)(light charged particle)-coin, (evaporation residue)(light charged particle)-coin; deduced source velocity, impact parameter dependence of preequilibrium particle emission.

doi: 10.1103/PhysRevC.48.291
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1992CZ01      Nucl.Phys. A542, 278 (1992)

J.Czakanski, W.Zipper, M.Siemaszko, W.Dunnweber, W.Hering, D.Konnerth, W.Trombik, K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Vandenbosch

Critical Angular Momentum of Cluster Evaporation: 16O(16O, α)28Si and 16O(16O, 8Be)24Mg

NUCLEAR REACTIONS 16O(16O, α), (16O, 8Be), E(cm)=18.35-31.0 MeV; measured σ(θ) vs E; deduced angular momentum limitation for cluster emission. Hauser-Feshbach model calculations with potential-barrier penetration coefficients.

doi: 10.1016/0375-9474(92)90217-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1257.

1991GI01      Phys.Rev. C43, 701 (1991)

S.Gil, R.Vandenbosch, A.Charlop, A.Garcia, D.D.Leach, S.J.Luke, S.Kailas

Spin Distribution of the Compound Nucleus Formed by 16O + 154Sm

NUCLEAR REACTIONS, ICPND 167Er(3He, n), (3He, 4n), (3He, X), E=27.2 MeV; 166Er(α, 2n), (α, 4n), (α, X), E=38.6, 43.1 MeV; 154Sm(16O, X), E=72 MeV; measured γ multiplicities, fusion, reaction σ; deduced compound nucleus spin distribution.

doi: 10.1103/PhysRevC.43.701
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1991LU03      Phys.Rev. C44, 1548 (1991)

S.J.Luke, C.A.Gossett, R.Vandenbosch

Search for High Energy γ Rays from the Spontaneous Fission of 252Cf

RADIOACTIVITY 252Cf(SF); measured γγ-, fission fragment(γ)-coin; deduced γ-production mechanism. Classical model, fission fragment Coulomb acceleration.

doi: 10.1103/PhysRevC.44.1548
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14544.

1990GI07      Phys.Rev.Lett. 65, 3100 (1990)

S.Gil, D.Abriola, D.E.DiGregorio, M.diTada, M.Elgue, A.Etchegoyen, M.C.Etchegoyen, J.Fernandez Niello, A.M.J.Ferrero, A.O.Macchiavelli, A.J.Pacheco, J.E.Testoni, P.Silveira-Gomes, V.R.Vanin, A.Charlop, A.Garcia, S.Kailas, S.J.Luke, E.Renshaw, R.Vandenbosch

Observation of Mean-Spin Barrier Bump in Sub-Barrier Fusion of 28Si with 154Sm

NUCLEAR REACTIONS, ICPND 154Sm(28Si, X), E=107-144 MeV; 166Er(16O, X), E=75-100 MeV; measured γ-multiplicity; deduced fusion σ(E). 182Os deduced spin distribution first moment vs E.

doi: 10.1103/PhysRevLett.65.3100
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1990KA28      Phys.Rev. C42, 2239 (1990)

S.Kailas, R.Vandenbosch, A.Charlop, S.J.Luke, D.Prindle, S.Van Verst

Fission Angular Distributions for the Systems 9Be + 232Th, 235U

NUCLEAR REACTIONS 232Th, 235U(9Be, F), E=50-53 MeV; measured fission fragment σ(θ); deduced fission σ. Statistical model analysis.

doi: 10.1103/PhysRevC.42.2239
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6093.

1990KA37      Pramana 35, 439 (1990)

S.Kailas, R.Vandenbosch, A.Charlop, A.Garcia, S.Gil, S.J.Luke, B.McLain, D.Prindle

Fusion Cross Section for the System 6Li + 28Si at E ≈ 36 MeV

NUCLEAR REACTIONS, ICPND 28Si(6Li, α), (6Li, p), (6Li, d), E ≈ 36 MeV; measured σ(θα, Eα), σ(θp, Ep), σ(θd, Ed). 28Si(6Li, X), E ≈ 36 MeV; measured fusion σ; deduced nucleus-nucleus potential.

doi: 10.1007/BF02846901
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1811.

1988RA40      Nucl.Phys. A490, 418 (1988)

J.Randrup, R.Vandenbosch

Hard Photon Production in the Nucleon-Exchange Transport Model

NUCLEAR REACTIONS Cu, Pb, 27Al(p, γ), E=140 MeV; calculated bremsstrahlung σ(E(γ), θ(γ)). 197Au(40Ar, X), E=30 MeV/nucleon; 158Gd(40Ar, X), 12C, Ag, 197Au(86Kr, X), E=44 MeV/nucleon; measured σ(θ(γ), E(γ)). Transport model.

doi: 10.1016/0375-9474(88)90513-1
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1988VA05      Phys.Rev. C37, 1301 (1988)

R.Vandenbosch, R.C.Connolly, S.Gil, D.D.Leach, T.C.Awes, S.Sorensen, C.Y.Wu

Light-Particle Multiplicity Accompanying Projectile Breakup at 20 MeV/Nucleon

NUCLEAR REACTIONS 181Ta(35Cl, X), (35Cl, αX), E=700 MeV; measured p(fragment)(fragment)-, α(fragment)(fragment)-coin; deduced α-, p-multiplicity.

doi: 10.1103/PhysRevC.37.1301
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1987CZ02      Phys.Lett. 199B, 166 (1987)

J.Czakanski, W.Zipper, W.Dunnweber, W.Hering, D.Konnerth, W.Trombik, K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Vandenbosch

Angular Momentum Limitation of Cluster Emission from the Compound Nucleus: 16O(16O, α)28Si and 16O(16O, 8Be)24Mg

NUCLEAR REACTIONS, MECPD 16O(16O, α), (16O, 8Be), E=36-62 MeV; measured σ(θ) vs E. Si detectors. Hauser-Feshbach model.

doi: 10.1016/0370-2693(87)91352-9
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1987RA34      Nucl.Phys. A474, 219 (1987)

J.Randrup, R.Vandenbosch

Pre-Equilibrium Neutron Emission in the Nucleon Exchange Transport Model

NUCLEAR REACTIONS 165Ho(20Ne, xn), E=402 MeV; calculated preequilibrium neutron multiplicity vs inital angular momentum, σ(θn, En). 238U(n, F), E=310 MeV; calculated σ(θn, En) following fission.

doi: 10.1016/0375-9474(87)90201-6
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1986MU01      Phys.Rev. C33, 165 (1986)

M.J.Murphy, D.Leach, A.Ray, A.Seamster, R.Vandenbosch

Decay of Excited Projectile Residues into Complex Fragments

NUCLEAR REACTIONS Ta(35Cl, X), E=20 MeV/nucleon; measured (fragment)(fragment)-coin, inclusive yield for fragment Z=10-16.

doi: 10.1103/PhysRevC.33.165
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1986MU13      Phys.Rev. C34, 1353 (1986)

T.Murakami, C.-C.Sahm, R.Vandenbosch, D.D.Leach, A.Ray, M.J.Murphy

Fission Probes of Sub-Barrier Fusion Cross Section Enhancements and Spin Distribution Broadening

NUCLEAR REACTIONS, ICPND 236U(12C, F), E=60-68 MeV; 208Pb, 232Th(16O, F), E=77-86 MeV; measured fission σ(E), σ(fragment θ), σ(fragment) vs mass. 208Pb, 232Th, 236U deduced quadrupole, octupole vibrational state parameters β, B(λ). 248Cf deduced mean-square spin distribution. Enriched targets, TOF telescope. Optical model and coupled channels calculations.

doi: 10.1103/PhysRevC.34.1353
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1396.

1986RA08      Phys.Rev.Lett. 57, 815 (1986)

A.Ray, D.D.Leach, R.Vandenbosch, K.T.Lesko, D.Shapira

Nonequilibrium Population of Magnetic Substates and Excitation-Energy Division in the Decay of an Orbiting Complex

NUCLEAR REACTIONS 12C(28Si, 12C), E(cm)=42.7, 33.7 MeV; measured γγ(θ), (particle)γ-coin, Eγ, Iγ; deduced orbiting complex decay excitation energy division. 12C level deduced m=0 magnetic substate production.

doi: 10.1103/PhysRevLett.57.815
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1986VA09      Phys.Rev.Lett. 56, 1234 (1986)

R.Vandenbosch, T.Murakami, C.-C.Sahm, D.D.Leach, A.Ray, M.J.Murphy

Anomalously Broad Spin Distributions in Sub-barrier Fusion Reactions

NUCLEAR REACTIONS 236U(12C, F), E=62, 66 MeV; 232Th(16O, F), E=85.7 MeV; measured fission fragment σ(θ). 248Cf deduced mean square spin value.

doi: 10.1103/PhysRevLett.56.1234
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1985GI04      Phys.Rev. C31, 1752 (1985)

S.Gil, R.Vandenbosch, A.J.Lazzarini, D.-K.Lock, A.Ray

Spin Distribution of the Compound Nucleus in Heavy Ion Reactions at Near-Barrier Energies

NUCLEAR REACTIONS, ICPND 154Sm(12C, xn), E=53 MeV; measured Eγ, Iγ, γγ-coin, γ-multiplicity. 154Sm(α, xn), E ≈ near barrier; measured γ-multiplicity. 154Sm(12C, 4n), E=46.7-60.7 MeV; 154Sm(α, n), E=15-24 MeV; measured γ multiplicity; deduced σ(E), fusion σ(E). 150Nd(16O, 3n), E ≈ 60-76 MeV; 150Nd(16O, 4n), E ≈ 60-84 MeV; 150Nd(16O, 5n), E=64-88 MeV; 154Sm(12C, X), E=47-61 MeV; 154Sm(α, X), E=14-24 MeV; analyzed relative yields, fusion σ(E). 170Yb, 166Er, 158Gd deduced spin distribution.

doi: 10.1103/PhysRevC.31.1752
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0416.

1985LO07      Phys.Rev. C31, 1268 (1985)

D.-K.Lock, R.Vandenbosch, J.Randrup

Transport and Evaporation Model Calculation of N and Z Distributions for Damped Nuclear Reactions

NUCLEAR REACTIONS 238U, 56Fe(56Fe, X), E=465 MeV; calculated fragment distribution charge, neutron number variances. Nucleon exchange model.

doi: 10.1103/PhysRevC.31.1268
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1985LO11      Nucl.Phys. A442, 142 (1985)

D.-K.Lock, R.Vandenbosch, K.Lesko, S.Gil, A.Seamster, D.Leach, A.Lazzarini

Nuclide Distributions for Fe-Like Fragments in the 136Xe + 56Fe Reaction

NUCLEAR REACTIONS 56Fe(136Xe, X), E=5.9 MeV/nucleon; measured σ(fragment, E, A), fragment yield vs mass charge, average values, variances, N-, Z-distributions, correlation coefficients vs energy loss.

doi: 10.1016/0375-9474(85)90138-1
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1985RA06      Phys.Rev. C31, 1573 (1985)

A.Ray, S.Gil, M.Khandaker, D.D.Leach, D.K.Lock, R.Vandenbosch

Entrance Channel Dependence of Back-Angle Yields: Orbiting in 24Mg + 16O reaction

NUCLEAR REACTIONS 16O(24Mg, 16O), (24Mg, 12C), E=79.5 MeV; measured σ(θ), energy spectra; deduced Q, evidence for orbiting. Compound nucleus model calculations.

doi: 10.1103/PhysRevC.31.1573
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1984MU21      Phys.Rev.Lett. 53, 1543 (1984)

M.J.Murphy, S.Gil, M.N.Harakeh, A.Ray, A.G.Seamster, R.Vandenbosch, T.C.Awes

Time Scale for Projectile Breakup into Coincident Heavy Fragments

NUCLEAR REACTIONS Ta(35Cl, X), E=680 MeV; measured (fragment)(fragment)-coin for Z=3-8; deduced sequential projectile breakup mechanism.

doi: 10.1103/PhysRevLett.53.1543
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1984VA10      Phys.Rev.Lett. 52, 1964 (1984)

R.Vandenbosch, A.Lazzarini, D.Leach, D.-K.Lock, A.Ray, A.Seamster

Nonequilibrium Excitation-Energy Division in Deeply Inelastic Collisions

NUCLEAR REACTIONS 238U(56Fe, F), E=8.5 MeV/nucleon; measured fission fragment total kinetic energy loss vs fragment mass; deduced heavy, light fragment excitation energy dependence.

doi: 10.1103/PhysRevLett.52.1964
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1983LE10      Phys.Rev. C27, 2999 (1983)

K.T.Lesko, S.Gil, A.Lazzarini, V.Metag, A.G.Seamster, R.Vandenbosch

Properties of Fission Induced by the Complete Capture of 40Ar by 238U at E(c.m.) = 291 MeV

NUCLEAR REACTIONS 238U(40Ar, F), E(cm)=291 MeV; measured fission fragment σ(θ); deduced complete capture induced fission characteristics. Rotating liquid drop model.

doi: 10.1103/PhysRevC.27.2999
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1983VA19      Phys.Rev. C28, 1161 (1983)

R.Vandenbosch, B.B.Back, S.Gil, A.Lazzarini, A.Ray

Penetration of the Centrifugal Barrier in the Fusion of 16O with Heavy Targets

NUCLEAR REACTIONS, ICPND 154Sm(16O, 4n), E=62.5-73.5 MeV; measured γ-multiplicity vs E; deduced fusion σ(E). 160Yb deduced rotational state deexcitation characteristics, ground state rotational band entry < J >.

doi: 10.1103/PhysRevC.28.1161
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1982LE04      Phys.Rev. C25, 872 (1982)

K.T.Lesko, D.-K.Lock, A.Lazzarini, R.Vandenbosch, V.Metag, H.Doubre

Energy Dependence of Fusion Cross Section for 28Si + 12C by Evaporation Residue Measurements

NUCLEAR REACTIONS, ICPND 28Si(12C, X)35Cl/38K/37Ar/34Cl/32S/34S/35Ar/35Cl/38Ar/31P, E(cm)=18.4-35 MeV; measured Eγ, Iγ, σ(evaporation residue) vs θ; deduced evaporation residual σ, fusion σ(E). Entrance channel, level density limitation models.

doi: 10.1103/PhysRevC.25.872
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1982ME05      Phys.Rev. C25, 1486 (1982)

V.Metag, A.Lazzarini, K.Lesko, R.Vandenbosch

Search for γ Rays from the Quasimolecular 12C + 12C System

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E(cm)=25.2 MeV; measured (12C)(12C)-, (12C)(12C)γ-coin. 24Mg resonances deduced γ-decay upper limit, characteristics.

doi: 10.1103/PhysRevC.25.1486
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1981BE29      Nucl.Phys. A365, 157 (1981)

K.G.Bernhardt, H.Bohn, K.A.Eberhard, R.Sielemann, R.Vandenbosch, M.P.Webb

The 12C(18O, α)26Mg and 12C(18O, 8Be)22Ne Reaction

NUCLEAR REACTIONS 12C(18O, 8Be), (18O, α), E(cm)=15-22.4 MeV; measured σ(E, θ); deduced no correlated structure. Statistical model calculations.

doi: 10.1016/0375-9474(81)90393-6
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1981LA03      Phys.Rev.Lett. 46, 988 (1981)

A.Lazzarini, V.Metag, A.G.Seamster, R.Vandenbosch, R.Loveman

Correlation of Aligned Angular Momentum with Scattering Angle and Energy Loss in Deeply Inelastic Collisions

NUCLEAR REACTIONS 165Ho(100Mo, X), E=450 MeV; measured γ-multiplicity, Iγ(φ) vs Q, σ(fragment θ) vs Q, total kinetic energy loss; deduced aligned angular momentum correlation with energy loss, θ. Surface barrier ΔE-E charged particle telescope, NaI(Tl) detector.

doi: 10.1103/PhysRevLett.46.988
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1981LA08      Phys.Rev. C24, 309 (1981)

A.Lazzarini, H.Doubre, K.T.Lesko, V.Metag, A.Seamster, R.Vandenbosch, W.Merryfield

Search for a Fusion L Window in the 16O + 16O System at E(cm) = 34 MeV

NUCLEAR REACTIONS 16O(16O, 16O'), E(cm)=34 MeV; measured σ(θ); deduced single, double excitation dominance. Comparison with TDHF.

doi: 10.1103/PhysRevC.24.309
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1981TS01      Phys.Rev. C23, 1560 (1981)

M.B.Tsang, W.G.Lynch, R.J.Puigh, R.Vandenbosch, A.G.Seamster

12C - α Angular Correlations in the 27Al(16O, 12Cα)27Al Reaction at 65 MeV

NUCLEAR REACTIONS 27Al(16O, α12C), E=65 MeV; measured σ(θ(12C), θα), 12Cα-coin. 31P deduced intermediate state equilibrium α-evaporation.

doi: 10.1103/PhysRevC.23.1560
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1981VA01      Phys.Rev.Lett. 46, 5 (1981)

R.Vandenbosch, D.-K.Lock, A.J.Lazzarini, K.Lesko, V.Metag

Nonresonant Behavior of the Yield of the 28Si 2+ (E(x)=1.78 MeV) State via the 12C + 28Si Reaction

NUCLEAR REACTIONS 28Si(12C, 12C'), E(cm)=23-35 MeV; measured Eγ, Iγ, σ(Eγ, E), σ(fusion, E), σ(E, θ(12C')). 28Si level deduced nonresonant total yield.

doi: 10.1103/PhysRevLett.46.5
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1980DY01      Phys.Rev. C22, 1509 (1980)

P.Dyer, M.P.Webb, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman

Charge Distributions for the 86Kr + 139La System at 506, 610, and 710 MeV

NUCLEAR REACTIONS 139La(86Kr, X), E=505, 610, 710 MeV; measured σ(fragment Z), σ(fragment θ, E, Z), fragment charge distribution variance vs energy loss; deduced combined fusion, fission σ, diffusion constants, reaction mechanism. Phenomenological model.

doi: 10.1103/PhysRevC.22.1509
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1980PU01      Nucl.Phys. A336, 279 (1980)

R.J.Puigh, H.Doubre, A.Lazzarini, A.Seamster, R.Vandenbosch, M.S.Zisman, T.D.Thomas

Alignment of Transferred Angular Momentum in Deeply Inelastic Collisions from Discrete γ-Ray Angular Correlations

NUCLEAR REACTIONS 166Er(86Kr, X), E=600 MeV; measured (fragment)γ-coin; deduced in-plane, out-of-plane yield of discrete γ, known multipolarity.

doi: 10.1016/0375-9474(80)90624-7
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1980VA03      Nucl.Phys. A339, 167 (1980)


On the Variations in Fusion Cross Sections for Different Light Heavy-Ion Systems

NUCLEAR REACTIONS 16O(10B, X), E(cm) ≈ 120-600 MeV; 14N(12C, X), E(cm)=100-700 MeV; calculated fusion σ(E). Classical trajectory model, proximity potential, electron scattering friction parameters.

doi: 10.1016/0375-9474(80)90248-1
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1979CH07      Phys.Rev.Lett. 42, 687 (1979)

Y.-d.Chan, H.Bohn, R.Vandenbosch, R.Sielemann, J.G.Cramer, K.G.Bernhardt, H.C.Bhang, D.T.C.Chiang

Influence of Extra Neutrons Added to the 12C + 16O System: Gross Structures in γ-Ray Yields Following the 13C + 16O and 12C + 18O Reactions

NUCLEAR REACTIONS 13C(16O, Xγ), 12C(18O, Xγ), E(cm)=7-25 MeV; measured σ(E, Eγ), Iγ. Compared structures in α-decay channels.

doi: 10.1103/PhysRevLett.42.687
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1979DY04      Nucl.Phys. A322, 205 (1979)

P.Dyer, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman, L.Nunnelley

Q- and Z-Dependence of Angular Momentum Transfer in Deeply Inelastic Collisions of 86Kr with 209Bi

NUCLEAR REACTIONS 209Bi(86Kr, F), E=610 MeV; measured σ(EF, θ, φ, Z).

doi: 10.1016/0375-9474(79)90342-7
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1979PU03      Phys.Lett. 86B, 24 (1979)

R.J.Puigh, P.Dyer, R.Vandenbosch, T.D.Thomas, L.Nunnelley, M.S.Zisman

Magnitude and Alignment of Transferred Angular Momentum in Both Quasi And Deeply Inelastic Scattering

NUCLEAR REACTIONS 238U(86Kr, F), E=730 MeV; measured projectile-like fragment, fission fragment (θ, φ); deduced magnitude, alignment of transferred as function of energy loss. Transport model.

doi: 10.1016/0370-2693(79)90612-9
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1979VA09      Phys.Rev. C20, 171 (1979)


Simple Model for Nuclear Alignment in Peripheral Nuclear Collisions

NUCLEAR REACTIONS 238U(86Kr, X), E=730 MeV; calculated alignment, magnitude of transfer angular momentum. Nucleon exchange model, effects of relative, internal motion for peripheral HI reactions.

doi: 10.1103/PhysRevC.20.171
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1979VA15      Phys.Lett. 87B, 183 (1979)


On the Origin of Oscillations in the Fusion Cross Section of 12C + 12C

NUCLEAR REACTIONS 12C(12C, X), E(cm)=6-22 MeV; calculated reaction, fusion σ(E); deduced oscillatory behavior related to availability of overlapping states of given L.

doi: 10.1016/0370-2693(79)90960-2
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1978CH15      Nucl.Phys. A303, 500 (1978)

Y.-D.Chan, H.Bohn, R.Vandenbosch, K.G.Bernhardt, J.G.Cramer, R.Sielemann, L.Green

Gross Structure in γ-Ray Yields Following the 16O + 12C Reaction

NUCLEAR REACTIONS 12C(16O, X), E=15-72 MeV; measured Iγ; deduced σ(E). Isotopic target.

doi: 10.1016/0375-9474(78)90373-1
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1978VA07      Phys.Rev. C17, 1672 (1978)

R.Vandenbosch, M.P.Webb, P.Dyer, R.J.Puigh, R.Weisfield, T.D.Thomas, M.S.Zisman

Elastic and Deeply Inelastic Reactions in the 86Kr + 139La System at 505, 610, and 710 MeV

NUCLEAR REACTIONS 139La(86Kr, 86Kr'), (86Kr, X), E=505, 610, 710 MeV; measured elastic, quasielastic, deep inelastic σ(θ), σ(E, θ) for non-elastic products. Elastic scattering optical model analysis.

doi: 10.1103/PhysRevC.17.1672
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1977BO21      Phys.Rev. C16, 665 (1977)

H.Bohn, K.A.Eberhard, R.Vandenbosch, K.G.Bernhardt, R.Bangert, Y-d.Chan

Back-Angle Anomalies in 6Li Scattering from 40Ca and 44Ca

NUCLEAR REACTIONS 40,44Ca(6Li, 6Li), (6Li, 6Li'), E=30 MeV; measured σ(θ). Optical model, coupled channel, Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.16.665
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1977DY04      Phys.Rev.Lett. 39, 392 (1977)

P.Dyer, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman

Angular-Momentum Transfer in Deeply Inelastic Scattering of 610-MeV 86Kr by 209Bi

NUCLEAR REACTIONS 209Bi(86Kr, X), E=610 MeV; measured fragment fragment (θ) from fission products.

doi: 10.1103/PhysRevLett.39.392
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1976VA04      Phys.Rev.Lett. 36, 459 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas

Energy Dependence of Deeply Inelastic Scattering of 84Kr from 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, 84Kr'), E=494, 510, 718 MeV; measured σ(E(84Kr'), θ).

doi: 10.1103/PhysRevLett.36.459
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1976VA11      Phys.Rev. C13, 1893 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas, S.W.Yates, A.M.Friedman

Elastic Scattering of 84Kr by 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, 84Kr), E=494, 510, 718 MeV; measured σ(θ). Fresnel, parametrized phase shift, optical model analyses.

doi: 10.1103/PhysRevC.13.1893
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1976VA12      J.Phys.(Paris), Lett. 37, L-161 (1976)

R.Vandenbosch, K.G.Bernhardt

How Strong Is the Absorption in the 12C + 20Ne System (Question)

NUCLEAR REACTIONS 12C(20Ne, 20Ne), 16O(16O, 16O), E(cm) ≈ 25 MeV; calculated potentials, σ(θ).

doi: 10.1051/jphyslet:01976003707-8016100
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1976VA15      Phys.Rev. C13, 143 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas

Deeply Inelastic Scattering of 84Kr from 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, X), E=494, 510, 718 MeV; measured σ(θ) for quasielastic, deeply inelastic scattering; deduced integrated σ, compared with optical model absorption σ. Deflection function analysis.

doi: 10.1103/PhysRevC.13.143
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1976VA18      Nucl.Phys. A269, 210 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas, M.S.Zisman

Energy, Angular and Charge Distributions for Deeply Inelastic Scattering of Xe by Ta and Pb

NUCLEAR REACTIONS 181Ta, 208Pb(136Xe, X), E=1120 MeV; measured σ(E, Z, θ).

doi: 10.1016/0375-9474(76)90407-3
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1976WE05      Phys.Rev.Lett. 36, 779 (1976)

M.P.Webb, R.Vandenbosch, K.A.Eberhard, K.G.Bernhardt, M.S.Zisman

18O + 12C System: Evidence for Nonstatistical Intermediate Structure with Enhancement of Odd Partial Waves in the Elastic Channel

NUCLEAR REACTIONS 12C(18O, 18O), (18O, 16O), (18O, α), E(cm)=12-25 MeV; measured σ(E, θ).

doi: 10.1103/PhysRevLett.36.779
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1976WE18      Phys.Lett. 62B, 407 (1976)

M.P.Webb, R.Vandenbosch, T.D.Thomas

Nuclear Reactions in the 86Kr + 139La System at 710 MeV

NUCLEAR REACTIONS 139La(86Kr, X), E=710 MeV; measured σ(θ); deduced reaction mechanism.

doi: 10.1016/0370-2693(76)90670-5
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1975RE15      Nucl.Phys. A253, 490 (1975)

W.N.Reisdorf, P.H.Lau, R.Vandenbosch

One-Neutron and Two-Neutron Transfer in the Scattering of 18O by 16O

NUCLEAR REACTIONS 16O(18O, 18O), E=42, 52 MeV; measured σ(θ). 16O(18O, 17O), E=42, 52 MeV; measured σ(E(17O), θ); deduced reaction mechanism.

doi: 10.1016/0375-9474(75)90494-7
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1975RU03      Nucl.Phys. A240, 13 (1975)

P.A.Russo, J.Pedersen, R.Vandenbosch

Gamma Decay of the 238U Shape Isomer

NUCLEAR REACTIONS 238U(d, npγ), E=13, 18 MeV; 238U(p, p'γ), E=13 MeV; measured σ(Eγ, t). 238U deduced levels, J, π, T1/2, barrier parameters.

doi: 10.1016/0375-9474(75)90434-0
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1974VA18      Phys.Rev.Lett. 33, 842 (1974)

R.Vandenbosch, M.P.Webb, M.S.Zisman

Entrance-Channel Effects in the 32S System: Comparison of 12C + 20Ne and 16O + 16O Elastic Scattering

NUCLEAR REACTIONS 20Ne(12C, 12C), E(cm)=17-28 MeV; measured σ(E); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.33.842
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1974VA22      Nucl.Phys. A230, 59 (1974)

R.Vandenbosch, W.N.Reisdorf, P.H.Lau

Elastic and Inelastic Scattering of 18O by 16O and 18O

NUCLEAR REACTIONS 16,18O(18O, 18O'), E=42, 52 MeV; measured σ(E(18O'), θ). 16,18O levels deduced deformation length.

doi: 10.1016/0375-9474(74)90529-6
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1973VA16      Phys.Rev. C8, 1080 (1973)

R.Vandenbosch, P.A.Russo, G.Sletten, M.Mehta

Relative Excitations of the 237Pu Shape Isomers

RADIOACTIVITY, Fission 237mPu(SF), 237Pu; measured delayed yields. 237Pu deduced levels, J, π, T1/2.

doi: 10.1103/PhysRevC.8.1080
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1973VA17      Phys.Lett. 45B, 207 (1973)


Influence of the Double Barrier on the Quadrupole Absorption Component Of Photofission

NUCLEAR REACTIONS, Fission 232Th, 240Pu(γ, F); calculated σ(E), fission barriers.

doi: 10.1016/0370-2693(73)90183-4
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1972BI15      Nucl.Phys. A198, 161 (1972)

C.J.Bishop, I.Halpern, R.W.Shaw, Jr., R.Vandenbosch

The Energy Dependence of the Fissionability of Neptunium Isotopes and the Level Density of Highly Deformed Nuclei

NUCLEAR REACTIONS, Fission 233U, 238U(p, xnF), E=11.5-22 MeV; measured (n)(fragment)(θ); ascribe deduced excitation energy dependence of n-width/t-width to deformation dependence of nuclear level density.

doi: 10.1016/0375-9474(72)90778-6
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1972RU03      Nucl.Phys. A188, 430 (1972)

C.Rudy, R.Vandenbosch, P.Russo, W.J.Braithwaite

Heavy-Ion Emission from Light Nuclei

NUCLEAR REACTIONS 12C, 16O(α, HI), HI=6Li, 7Li, 7Be, 8Be, 9Be, 10B, 11C, 12C, 13C, 13N, 14N, E=42 MeV; measured σ(θ). Statistical model comparison.

doi: 10.1016/0375-9474(72)90068-1
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1972VA08      Phys.Rev. C5, 1428 (1972)


Spontaneous-Fission-Isomer Excitation Energies from Threshold Measurements

doi: 10.1103/PhysRevC.5.1428
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1972VA15      Phys.Rev.Lett. 28, 1726 (1972)

R.Vandenbosch, U.Mosel

Single-Particle Effects on Fission Probabilities for the Lighter Elements

NUCLEAR STRUCTURE 210Po, 198Hg, 201Tl, 191Ir; analyzed single-particle effects on fission probabilities.

doi: 10.1103/PhysRevLett.28.1726
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1971RU03      Phys.Rev. C3, 1595 (1971)

P.A.Russo, R.Vandenbosch, M.Mehta, J.R.Tesmer, K.L.Wolf

Spin Isomers of the Shape Isomer 237mPu

RADIOACTIVITY, Fission 237mPu(SF); measured T1/2; deduced shape isomerism.

doi: 10.1103/PhysRevC.3.1595
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1970BI06      Nucl.Phys. A150, 129 (1970)

C.J.Bishop, R.Vandenbosch, R.Aley, R.W.Shaw, Jr., I.Halpern

Excitation Energy Dependence of Neutron Yields and Fragment Kinetic Energy Release in the Proton Induced Fission of 233U and 238U

NUCLEAR REACTIONS, Fission 233,238U(p, F), E=9.5-22 MeV; measured prompt neutron energies, yields(E;fragment mass).

doi: 10.1016/0375-9474(70)90462-8
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1970KA03      Phys.Rev. C1, 594 (1970)

A.A.Katsanos, R.W.Shaw, Jr., R.Vandenbosch, D.Chamberlin

Persistence of Odd-Even Effect on Nuclear Level Densities at High Excitation Energy

NUCLEAR REACTIONS 54Cr(p, α), E=6.5-20 MeV; measured σ(E;θ); deduced reaction mechanism. 55Mn deduced resonances, level-width, level density, autocorrelation function.

doi: 10.1103/PhysRevC.1.594
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1970RU11      Nucl.Phys. A159, 153 (1970)

P.A.Russo, R.Vandenbosch

Mass Determination of the Neutron-Deficient Nucleides 88Zr and 140Nd by (p, 2n) Threshold Measurements

NUCLEAR REACTIONS 141Pr(p, 2n), 89Y(p, 2n), E=10-15 MeV; measured σ(E); deduced thresholds, Q. 140Nd, 88Zr deduced mass excesses.

doi: 10.1016/0375-9474(70)90033-3
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1970SH07      Phys.Rev.Lett. 25, 457 (1970)

R.W.Shaw, Jr., R.Vandenbosch, M.K.Mehta

Elastic Scattering of 18O by 18O

NUCLEAR REACTIONS 18O(18O, 18O), E=7.5-27.5 MeV; measured σ(E).

doi: 10.1103/PhysRevLett.25.457
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1970WO06      Phys.Rev. C1, 2096 (1970)

K.L.Wolf, R.Vandenbosch, P.A.Russo, M.K.Mehta, C.R.Rudy

Spontaneous Fission Isomerism in Uranium Isotopes

RADIOACTIVITY, Fission 236mU, 238mU(SF); measured T1/2.

NUCLEAR REACTIONS 236,238U(d, X), (d, pn), E=13-22 MeV; measured σ(E;Ep). 236,238U deduced isomer ratios.

doi: 10.1103/PhysRevC.1.2096
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1969SH17      Phys.Rev. 184, 1040 (1969)

R.W.Shaw, Jr., J.C.Norman, R.Vandenbosch, C.J.Bishop

Energy and Angular Dependence of Differential Cross Sections for the 16O(16O, α)28Si Reaction

NUCLEAR REACTIONS 16O(16O, α), (16O, 16O), E=35-39 MeV; measured σ(E;Eα, θ(α)), σ(E;E(16O'), θ). 32S deduced resonances, level density, cross-, auto-correlations.

doi: 10.1103/PhysRev.184.1040
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1969SH18      Phys.Rev. 184, 1089 (1969)

R.W.Shaw, Jr., A.A.Katsanos, R.Vandenbosch

Experimental Test of Statistical-Model Approximations When Gamma/D > 1

NUCLEAR REACTIONS 27Al(p, α), E=8-10 MeV; measured σ(E;θ). 28Si deduced resonances, level-width, autocorrelations.

doi: 10.1103/PhysRev.184.1089
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1968RU10      J.Inorg.Nucl.Chem. 30, 365 (1968)

C.Rudy, R.Vandenbosch, C.T.Ratcliffe

Relative Independent Yields for 95Nb and 95mNb from Low Energy Fission

NUCLEAR REACTIONS, Fission 235U(p, F), E=10 MeV; measured isomeric σ ratio, 95Nb, 95mNb independent yields.

doi: 10.1016/0022-1902(68)80462-2
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1967VA18      Phys.Rev. 158, 887 (1967)

R.Vandenbosch, J.C.Norman, C.J.Bishop

Si28(He4, O16)O16 Reaction

NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.158.887
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1966BI11      Nucl.Phys.Lab., Univ.Washington, Annual Rept., p.20 (June 1966)

C.J.Bishop, R.Vandenbosch

The Cu63(d, He3)Ni62 Reaction

NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.

1965BI13      Univ.Washington Annual Rept., Nucl.Phys.Lab., p.31 (1965)

C.J.Bishop, R.Vandenbosch

Cu63(d, α)Ni61 and Cu63(d, He3)Ni62 Reactions

NUCLEAR STRUCTURE 62Ni, 61Ni; measured not abstracted; deduced nuclear properties.

1964VA04      J.Inorg.Nucl.Chem. 26, 219 (1964)

R.Vandenbosch, P.R.Fields, S.E.Vandenbosch, D.Metta

Search for a Spontaneous Fission Branch in a Metastable State of Cm244

NUCLEAR STRUCTURE, Fission 244Cm; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(64)80061-0
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1964WA10      J.Inorg.Nucl.Chem. 26, 669 (1964)

H.Warhanek, R.Vandenbosch

Relative Cross-Sections for Formation of the Shielded Isomeric Pair 134mCs and 134Cs in Medium Energy Fission

NUCLEAR STRUCTURE, Fission 134Cs; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(64)80308-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2559.

1963SC35      Phys.Lett. 5, 292 (1963)

J.P.Schiffer, R.Vandenbosch

Search for a Particle-Stable Tetra Neutron

doi: 10.1016/S0375-9601(63)96134-6
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1962HU14      Nucl.Phys. 34, 439 (1962)

J.R.Huizenga, K.M.Clarke, J.E.Gindler, R.Vandenbosch

Photofission Cross Sections Of Several Nuclei With Mono-Energetic Gamma Rays

NUCLEAR REACTIONS 232Th(γ, f), 233U(γ, f), 234U(γ, f), 235U(γ, f), 236U(γ, f), 238U(γ, f), 237Np(γ, f), E=6.1-7 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry M0505.

doi: 10.1016/0029-5582(62)90231-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0505.

1962HU15      Phys.Rev. 126, 210 (1962)

J.R.Huizenga, R.Chaudhry, R.Vandenbosch

Helium-Ion-Induced Fission of Bi, Pb, Tl, and Au

NUCLEAR REACTIONS 197Au, 203Tl, 206Pb, 209Bi(α, f), E=34.3-43 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry P0093.

doi: 10.1103/PhysRev.126.210
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetP0093.

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