NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.Vandenbosch Found 111 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1994VA27 Phys.Rev. C50, 2618 (1994) Origin of Empirical Threshold for Disspiative Fission
doi: 10.1103/PhysRevC.50.2618
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
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
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
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
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
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
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
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
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
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
1988RA40 Nucl.Phys. A490, 418 (1988) 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
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
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
1987RA34 Nucl.Phys. A474, 219 (1987) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1976VA12 J.Phys.(Paris), Lett. 37, L-161 (1976) 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
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
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
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
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
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
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
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
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
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
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
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
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
1972VA08 Phys.Rev. C5, 1428 (1972) Spontaneous-Fission-Isomer Excitation Energies from Threshold Measurements
doi: 10.1103/PhysRevC.5.1428
1972VA15 Phys.Rev.Lett. 28, 1726 (1972) 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
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
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
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
1970RU11 Nucl.Phys. A159, 153 (1970) 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
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
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
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
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
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
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
1966BI11 Nucl.Phys.Lab., Univ.Washington, Annual Rept., p.20 (June 1966) 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) 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
1964WA10 J.Inorg.Nucl.Chem. 26, 669 (1964) 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
1963SC35 Phys.Lett. 5, 292 (1963) Search for a Particle-Stable Tetra Neutron
doi: 10.1016/S0375-9601(63)96134-6
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
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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