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NSR database version of April 11, 2024.

Search: Author = M.S.Zisman

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1989PE01      Phys.Rev. C39, 488 (1989)

G.F.Peaslee, N.N.Ajitanand, J.M.Alexander, R.Lacey, L.C.Vaz, M.Kaplan, M.Kildir, D.J.Moses, D.Logan, M.S.Zisman

Particle-Particle Coincidence Measurements for 1,2,3H and 4He in the Reaction 480 MeV 56Fe + (nat)Ag

NUCLEAR REACTIONS Ag(56Fe, pX), (56Fe, dX), (56Fe, tX), (56Fe, αX), E=480 MeV; measured (particle)(particle)-coin; deduced average particle multiplicities, energy removed, effective emission barriers.

doi: 10.1103/PhysRevC.39.488
Citations: PlumX Metrics


1988LA12      Phys.Rev. C37, 2540 (1988)

R.Lacey, N.N.Ajitanand, J.M.Alexander, D.M.de Castro Rizzo, G.F.Peaslee, L.C.Vaz, M.Kaplan, M.Kildir, G.La Rana, D.J.Moses, W.E.Parker, D.Logan, M.S.Zisman, P.DeYoung, L.Kowalski

Mechanisms for Light Charged Particle Emission in the Reactions 247 and 337 MeV 40Ar + (nat)Ag

NUCLEAR REACTIONS Ag(40Ar, pX), (40Ar, dX), (40Ar, tX), (40Ar, αX), (40Ar, X), E=247, 337 MeV; measured σ(θ), σ(Eα, θα); deduced pre-, post scission emission multiplicities. Deformed emitters.

doi: 10.1103/PhysRevC.37.2540
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1988LA13      Phys.Rev. C37, 2561 (1988)

R.Lacey, N.N.Ajitanand, J.M.Alexander, D.M.de Castro Rizzo, G.F.Peaslee, L.C.Vaz, M.Kaplan, M.Kildir, G.La Rana, D.J.Moses, W.E.Parker, D.Logan, M.S.Zisman, P.DeYoung, L.Kowalski

Large-Angle Correlations between 4He and 1,2,3H or 4He in the Reactions 247 and 337 MeV 40Ar + (nat)Ag: Unexpected properties of the nuclear stratosphere

NUCLEAR REACTIONS Ag(40Ar, αX), E=247, 337 MeV; measured α(light fragment)-coin, energy correlations; deduced emission source properties, mechanism.

doi: 10.1103/PhysRevC.37.2561
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1988PE16      Phys.Rev. C38, 1730 (1988)

G.F.Peaslee, N.N.Ajitanand, J.M.Alexander, D.Guerreau, R.Lacey, L.C.Vaz, M.Kaplan, M.Kildir, D.J.Moses, D.Logan, M.S.Zisman

Sources of Light-Charged-Particle Emission in the Reaction 480 MeV 56Fe + (nat)Ag

NUCLEAR REACTIONS Ag(56Fe, pX), (56Fe, dX), (56Fe, tX), (56Fe, αX), E=480 MeV; measured σ(fragment θ), σ(E(X), θ(X)) for X=p, d, t, α; deduced reaction, particle emission mechanisms.

doi: 10.1103/PhysRevC.38.1730
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1987MO05      Nucl.Phys. A465, 339 (1987)

D.J.Moses, M.Kaplan, M.Kildir, D.R.G.Logan, G.La Rana, W.E.Parker, R.Lacey, G.F.Peaslee, J.M.Alexander, N.N.Ajitanand, L.C.Vaz, M.S.Zisman

Light Charged Particle Emission in 485 MeV 56Fe + 197Au Reactions: Correlations with heavy fragments and relationships to spin and lifetime

NUCLEAR REACTIONS 197Au(56Fe, X), (56Fe, F), E=485 MeV; measured σ(Eα, θα, fragment θ), σ(Ep), σ(Eα), σ(Ep, θp, fragment θ) following fission, deep inelastic scattering; deduced evaporative light-particle multiplicities for each emission source. 252Db deduced T1/2.

doi: 10.1016/0375-9474(87)90438-6
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1985MO04      Z.Phys. A320, 229 (1985)

D.J.Moses, M.Kaplan, J.M.Alexander, D.Logan, M.Kildir, L.C.Vaz, N.N.Ajitanand, E.Duek, M.S.Zisman

Particle Spectra from Reversed Kinematics: Powerful probes of hot rotating nuclei

NUCLEAR REACTIONS 12C(40Ar, pX), (40Ar, αX), (56Fe, pX), (56Fe, αX), (86Kr, pX), (86Kr, αX), E=8.5 MeV/nucleon; measured inclusive σ(θ, Ep), σ(θ, Eα); deduced effective evaporation emission, fusion barriers. Hot spot, moving source model.

doi: 10.1007/BF01881270
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1984AJ02      Z.Phys. A316, 169 (1984)

N.N.Ajitanand, J.M.Alexander, H.Delagrange, E.Duek, D.O.Eriksen, D.Guerreau, M.Kaplan, M.Kildir, L.Kowalski, R.Lacey, D.Logan, D.J.Moses, G.F.Peaslee, L.C.Vaz, M.S.Zisman

Multiplicities for Evaporative 4He Emission in Heavy Ion Reactions: Relationships to spin and lifetime expectancy of the composite nucleus

NUCLEAR REACTIONS Ag, 238U(40Ar, αX), (56Fe, αX), (40Ar, αF), (56Fe, αF), E=8.5 MeV/nucleon; measured σ(fragment θ, θα, Eα), fission-fusion, projectile-like fragment-coin; deduced reaction mechanism, hot nucleus thermodynamic properties.

doi: 10.1007/BF01412259
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1984DU09      Z.Phys. A317, 83 (1984)

E.Duek, N.N.Ajitanand, J.M.Alexander, D.Logan, M.Kildir, L.Kowalski, L.C.Vaz, D.Guerreau, M.S.Zisman, M.Kaplan, D.J.Moses

Mechanisms for Emission of 4He in the Reactions of 334 MeV 40Ar with 238U

NUCLEAR REACTIONS 238U(40Ar, αF), E=334 MeV; measured fission (fragment)(fragment)(α)-coin, σ(θα, Eα); deduced fission, α-emission mechanisms.

doi: 10.1007/BF01420452
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1984KI07      Z.Phys. A317, 291 (1984)

M.Kildir, D.Logan, D.O.Eriksen, D.J.Moses, M.Kaplan, E.Duek, L.C.Vaz, N.N.Ajitanand, J.M.Alexander, M.S.Zisman

Fission Reactions of 468-MeV 56Fe + 238U: Detection of 4He/1H Emission from Pre- and Post-Fission Sources

NUCLEAR REACTIONS 238U(56Fe, pF), (56Fe, αF), E=469 MeV; measured fission (fragment)(fragment)(θ), σ(θp, Ep, fragment θ), σ(θα, Eα, fragment θ), proton, α differential multiplicities, σ(θα, Eα); deduced light particle emission mechanism.

doi: 10.1007/BF01438361
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1984VA05      Z.Phys. A315, 169 (1984)

L.C.Vaz, D.Logan, E.Duek, J.M.Alexander, M.F.Rivet, M.S.Zisman, M.Kaplan, J.W.Ball

Fission and Emission of H and He in the Reactions of 215 MeV 16O with 181Ta, 208Pb and 238U

NUCLEAR REACTIONS 12C, 181Ta, 208Pb, 238U(16O, pX), (16O, αX), E=215 MeV; 181Ta, 208Pb, 238U(16O, dX), (16O, tX), E=215 MeV; measured inclusive σ(Ep), σ(Eα), σ(Ed), σ(Et), σ(θ), σ(θ, Ep), σ(θ, Eα). 209Bi, 238U(16O, F), E=215 MeV; measured fission σ; deduced evaporative emission effective barriers.

doi: 10.1007/BF01419376
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1983DU14      Phys.Lett. 131B, 297 (1983)

E.Duek, N.N.Ajitanand, J.M.Alexander, D.Logan, M.Kildir, L.Kowalski, L.C.Vaz, D.Guerreau, M.S.Zisman, M.Kaplan

New Probe of Interediate Reaction Times: Near-Scission Emission of 4He for 334 MeV 40Ar + 238U

NUCLEAR REACTIONS 238U(40Ar, αX), (40Ar, αF), E= 334 MeV; measured α(fragment)-coin following fusion, fission; deduced fragment, composite nucleus evaporation upper limit, near scission role.

doi: 10.1016/0370-2693(83)90502-6
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1983KA16      Z.Phys. A313, 31 (1983)

M.Kaplan, D.J.Moses, D.O.Eriksen, M.Kildir, D.R.G.Logan, M.S.Zisman, R.J.McDonald

Light Charged Particle Emission and Fission in 238U + 238U Collisions at 1, 740 MeV

NUCLEAR REACTIONS 197Au, 238U(238U, pX), (238U, αX), E=7.31 MeV/nucleon; measured p(fragment)-, α(fragment)-coin, σ(θp, Ep), σ(θα, Eα); deduced reaction mechanism, target, projectile sequential fission.

doi: 10.1007/BF02115840
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1983VA10      Z.Phys. A311, 89 (1983)

L.C.Vaz, D.Logan, J.M.Alexander, E.Duek, D.Guerreau, L.Kowalski, M.F.Rivet, M.S.Zisman

Products of 3 ≤ Z ≤ 9 from Long-Lived Intermediates in the Reactions 336 MeV 40Ar + Ag, 154Sm and Au

NUCLEAR REACTIONS 107,109Ag, 197Au, 154Sm(40Ar, 7Li), (40Ar, 9Be), (40Ar, 11B), (40Ar, 12C), (40Ar, 14N), (40Ar, 16O), (40Ar, 19F), E=336 MeV; measured σ(fragment θ), σ(fragment θ, E); deduced fission σ, σ(evaporation residue), σ(fusion), σ(reaction). 149Tb, 194Hg deduced effective emission barriers, rms spin values. Semi-classical analysis.

doi: 10.1007/BF01411611
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1982DU09      Z.Phys. A307, 221 (1982)

E.Duek, L.Kowalski, M.Rajagopalan, J.M.Alexander, D.Logan, M.S.Zisman, M.Kaplan

Correlations between Fission Fragments for 172 MeV 20Ne + 197Au: A case study for incomplete fusion

NUCLEAR REACTIONS 197Au(20Ne, F), E=172 MeV; measured fission (fragment)(fragment)(θ), total kinetic energy, mean mass vs θ, linear momentum transfer; deduced reaction mechanism. Monte Carlo calculation.

doi: 10.1007/BF01438643
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1982KI06      Z.Phys. A306, 323 (1982)

M.Kildir, D.Logan, M.Kaplan, M.S.Zisman, D.Guerreau, J.M.Alexander, L.C.Vaz

Studies of 4He Emission in Both Fusion-Like and Inelastic Reactions of 340-MeV 40Ar + 238U

NUCLEAR REACTIONS 238U(40Ar, αF), E=340 MeV; measured σ(θα, Eα), (fragment)(fragment)α-coin; deduced fusion-fission, sequential fission induced direct, evaporation α emission.

doi: 10.1007/BF01432373
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1982RA06      Phys.Rev. C25, 2417 (1982)

M.Rajagopalan, D.Logan, J.W.Ball, M.Kaplan, H.Delagrange, M.F.Rivet, J.M.Alexander, L.C.Vaz, M.S.Zisman

Charged Particle Emission from 194Hg Compound Nuclei: Energy and spin dependence of fission-evaporation competition

NUCLEAR REACTIONS, ICPND 182W(12C, F), (12C, p), (12C, d), (12C, t), (12C, α), E=77-167 MeV; 175Lu(19F, F), (19F, p), (19F, d), (19F, t), (19F, α), E=135, 184 MeV; 174Yb(20Ne, F), (20Ne, p), (20Ne, d), (20Ne, t), (20Ne, α), E=125, 252 MeV; 154Sm(40Ar, F), (40Ar, p), (40Ar, d), (40Ar, t), (40Ar, α), E=196-340 MeV; measured σ(E), fission σ, fusion σ, evaporation residue σ vs E; deduced reaction mechanism. 194Hg deduced fission, evaporation competition spin, energy dependences. Statistical model.

doi: 10.1103/PhysRevC.25.2417
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1982RI02      Phys.Rev. C25, 2430 (1982)

M.F.Rivet, D.Logan, J.M.Alexander, D.Guerreau, E.Duek, M.S.Zisman, M.Kaplan

Energy Equilibration in Composite Nuclei at High Energy and Spin: Correlations between evaporative 1H, 4He, and fission

NUCLEAR REACTIONS, Fission 116Sn, 154Sm, 197Au(40Ar, pF), (40Ar, dF), (40Ar, tF), (40Ar, αF), E=333 MeV; measured (fragment)p-, (fragment)d-, (fragment)t-, (fragment)α-coin, σ(fragment θ, θp, Ep), σ(fragment θ, θα, Eα); deduced reaction mechanism. 237Bk, 194Hg, 156Er deduced emission barriers, level density parameters, rms(J). Evaporation, statistical models.

doi: 10.1103/PhysRevC.25.2430
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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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1980LO08      Phys.Rev. C22, 104 (1980)

D.Logan, M.Rajagopalan, M.S.Zisman, J.M.Alexander, M.Kaplan, L.Kowalski

Rapid Energy Equilibration and Emission of H and He in the Reaction of 340-MeV 40Ar with 197Au

NUCLEAR REACTIONS 197Au(40Ar, F), (40Ar, p), (40Ar, d), (40Ar, t), (40Ar, α), E=340 MeV; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(Eα, θα), light particle fission fragment-coin; deduced reaction mechanism. 237Bk deduced average spin, equilibration parameters.

doi: 10.1103/PhysRevC.22.104
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0358.


1980LO11      Phys.Rev. C22, 1080 (1980)

D.Logan, H.Delagrange, M.F.Rivet, M.Rajagopalan, J.M.Alexander, M.Kaplan, M.S.Zisman, E.Duek

Light-Charged-Paricle Emission in 40Ar-Induced Reactions: A Probe of the Very Early Evolution of the Collisions

NUCLEAR REACTIONS, Fission 116Sn, 154Sm, 164Dy, 197Au(40Ar, p), (40Ar, α), (40Ar, F), (40Ar, X), E=222, 274, 340 MeV; measured σ(fragment, θ), (fragment)p-, (fragment)α-coin; deduced rapid energy thermalization, production s(θ) for Li, Be, B, C, N, O.

doi: 10.1103/PhysRevC.22.1080
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0358.


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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1980ZI02      Phys.Rev. C21, 2398 (1980)

M.S.Zisman, J.G.Cramer, D.A.Goldberg, J.W.Watson, R.M.DeVries

Dominance of Strong Absorption in 9Be + 28Si Elastic Scattering

NUCLEAR REACTIONS 28Si(9Be, 9Be), E=121, 201.6 MeV; measured σ(θ); deduced Woods-Saxon, proximity optical model parameters, fusion barriers, strong absorption effects.

doi: 10.1103/PhysRevC.21.2398
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1979BR01      Phys.Rev. C19, 9 (1979)

G.Bruge, M.S.Zisman, A.D.Bacher, R.Schaeffer, C.J.Zeippen, J.M.Loiseaux

(3He, t) Reaction Mechanism via the 38Ar(3He, t)38K Reaction at 40 Mev

NUCLEAR REACTIONS 38Ar(3He, t), E=40 MeV; measured σ(θ). 38K levels deduced L, strength of microscopic (3He, t) force. Microscopic DWBA. Coupled-channels analysis.

doi: 10.1103/PhysRevC.19.9
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1979DE32      Phys.Rev.Lett. 43, 1490 (1979)

H.Delagrange, D.Logan, M.F.Rivet, M.Rajagopalan, J.M.Alexander, M.S.Zisman, M.Kaplan, J.W.Ball

Fusion and Emission of 1H and 4He in Reactions between Complex Nuclei At High Energies

NUCLEAR REACTIONS 116Sn, 154Sm, 164Dy, 197Au(40Ar, p), (40Ar, α), (40Ar, X), (40Ar, F), E=222-340 MeV; 182W(12C, X), E=77-167 MeV; 116Sn(40Ar, X), E=187 MeV; measured σ(θ), fusion, fission σ(E).

doi: 10.1103/PhysRevLett.43.1490
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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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1979RA01      Phys.Rev. C19, 54 (1979)

M.Rajagopalan, L.Kowalski, D.Logan, M.Kaplan, J.M.Alexander, M.S.Zisman, J.M.Miller

Coincidence Studies of Heavy Fragments in Deeply Inelastic Collisions Between Heavy Ions: Sequential Fission Probability in Reactions of 730-MeV 86Kr with Au

NUCLEAR REACTIONS 197Au(86Kr, X), E=730 MeV; measured (fragment)(fragment)-coin, correlation; deduced sequential fission probability as a function of inelastic energy transfer.

doi: 10.1103/PhysRevC.19.54
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1979VI13      Phys.Rev. C20, 2147 (1979)

S.E.Vigdor, D.G.Kovar, P.Sperr, J.Mahoney, A.Menchaca-Rocha, C.Olmer, M.S.Zisman

Energy Dependence of the Fusion and Elastic Scattering of 16O + 40Ca

NUCLEAR REACTIONS 40Ca(16O, 16O), (16O, X), E=40-214 MeV; measured fusion σ(E), elastic σ(θ, E); deduced S-wave barrier parameters, optical model parameters, fusion mechanisms.

doi: 10.1103/PhysRevC.20.2147
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1978KE06      Phys.Rev. C17, 1929 (1978)

G.J.KeKelis, M.S.Zisman, D.K.Scott, R.Jahn, D.J.Vieira, J.Cerny, F.Ajzenberg-Selove

Masses of the Unbound Nuclei 16Ne, 15F, and 12O

NUCLEAR REACTIONS 16O, 20Ne(α, 8He), E=117 MeV; 20Ne(3He, 8Li), E=75, 88 MeV; measured σ(θ); deduced Q. 12O, 15F, 16Ne deduced mass excess, Γ(cm), diproton decay.

doi: 10.1103/PhysRevC.17.1929
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1978MI01      Phys.Rev.Lett. 40, 100 (1978)

J.M.Miller, G.L.Catchen, D.Logan, M.Rajagopalan, J.M.Alexander, M.Kaplan, M.S.Zisman

Pre-Equilibrium α Emission in Reactions of 724-MeV 86Kr with Au: A Coincidence Study of Direct and Evaporation Mechanisms

NUCLEAR REACTIONS Au(84Kr, X), E=724 MeV; measured αHI-coin.

doi: 10.1103/PhysRevLett.40.100
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1978MI06      Phys.Rev.Lett. 40, 1074 (1978)

J.M.Miller, D.Logan, G.L.Catchen, M.Rajagopalan, J.M.Alexander, M.Kaplan, J.W.Ball, M.S.Zisman, L.Kowalski

Energy and Spin Dependence of Fission: 1H and 4He Emission from 194Hg Compound Nuclei

NUCLEAR REACTIONS 182W(12C, X), E=98 MeV; 175Lu(19F, X), E=142 MeV; measured σ(θ) for evaporation residues, fission, fusion, p-, α-emission.

doi: 10.1103/PhysRevLett.40.1074
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1978PI09      Phys.Rev. C18, 180 (1978)

S.C.Pieper, M.H.Macfarlane, D.H.Gloeckner, D.G.Kovar, F.D.Becchetti, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, F.Puhlhofer, W.von Oertzen, M.S.Zisman

Energy Dependence of Elastic Scattering and One-Nucleon Transfer Reactions Induced by 16O on 208Pb. I

NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-216.6 MeV; 208Pb(16O, 15N), (16O, 17O), E=104, 138.5, 216.6 MeV; measured σ(θ). Optical model, DWBA analysis.

doi: 10.1103/PhysRevC.18.180
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1978SA06      Nucl.Phys. A298, 313 (1978)

G.R.Satchler, M.L.Halbert, N.M.Clarke, E.E.Gross, C.B.Fulmer, A.Scott, D.Martin, M.D.Cohler, D.C.Hensley, C.A.Ludemann, J.G.Cramer, M.S.Zisman, R.M.DeVries

Heavy-Ion Elastic Scattering (II). 142 MeV 16O on 28Si, 59Co and 60Ni

NUCLEAR REACTIONS 28Si, 59Co, 60Ni(16O, 16O); 28Si, 60Ni(16O, 16O'), E=141.9 MeV; measured σ(θ); deduced optical potentials.

doi: 10.1016/0375-9474(78)90259-2
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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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1977DE23      Phys.Rev.Lett. 39, 450 (1977)

R.M.DeVries, D.A.Goldberg, J.W.Watson, M.S.Zisman, J.G.Cramer

Transition between Light- and Heavy-Ion Elastic Scattering

NUCLEAR REACTIONS 28Si(6Li, 6Li), E=135.1 MeV; 28Si(12C, 12C), E=186 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1103/PhysRevLett.39.450
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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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1977SH06      Phys.Rev. C15, 903 (1977)

J.D.Sherman, D.L.Hendrie, M.S.Zisman

Spectroscopy of 140Ce and 138Ce via the 140Ce(p, p'), 142Ce(p, t), and 140Ce(p, t) Reactions at E = 30 MeV

NUCLEAR REACTIONS 140Ce(p, p'), 142Ce(p, t), E=30 MeV; measured σ(θ). 140Ce(p, t), E=30 MeV; measured relative σ(Et, θ); deduced Q. 140,138Ce deduced levels, L, J, π.

doi: 10.1103/PhysRevC.15.903
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1977ST20      Phys.Rev. C16, 1456 (1977)

D.P.Stahel, G.J.Wozniak, M.S.Zisman, B.D.Jeltema, J.Cerny

(9Be, 8Be) Reaction at 50 MeV

NUCLEAR REACTIONS 12C, 16O, 26Mg, 28Si, 40Ca, 208Pb(9Be, 8Be), 12C, 28Si, 40Ca, 208Pb(9Be, 9Be), E=50 MeV; measured σ(θ). 13C, 17O, 27Mg, 29Si, 41Ca, 209Pb levels deduced relative, absolute S.

doi: 10.1103/PhysRevC.16.1456
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1977ST25      Phys.Lett. 70B, 289 (1977)

R.G.Stokstad, R.A.Dayras, J.Gomez del Campo, P.H.Stelson, C.Olmer, M.S.Zisman

Measurements of the Fusion of 12C + 14N and the Liquid-Drop Limit for 26Al

NUCLEAR REACTIONS 12C(14N, X), E=248 MeV; measured fusion σ.

doi: 10.1016/0370-2693(77)90660-8
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1977WE03      Nucl.Phys. A280, 217 (1977)

R.B.Weisenmiller, N.A.Jelley, D.Ashery, K.H.Wilcox, G.J.Wozniak, M.S.Zisman, J.Cerny

Very Light Neutron-Rich Nuclei Studied with the (6Li, 8B) Reaction

NUCLEAR REACTIONS 6Li(6Li, 8B), 7Li(6Li, 8B), 9Be(6Li, 8B), 11B(6Li, 8B), E=80.0, 93.3 MeV; measured σ(θ). 4H, 7He, 9Li deduced structure parameters.

doi: 10.1016/0375-9474(77)90305-0
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1976AS01      Phys.Rev. C13, 1345 (1976)

D.Ashery, M.S.Zisman, G.W.Goth, G.J.Wozniak, R.B.Weisenmiller, J.Cerny

T = 2 States in 12C and 12B

NUCLEAR REACTIONS 14C(p, t), (p, 3He), E=54 MeV; measured σ(θ). 14C(p, pt), (p, tα), E=54 MeV; measured pt-, tα-coin. 12C, 12B deduced IAS, J.

doi: 10.1103/PhysRevC.13.1345
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1976CR04      Phys.Rev. C14, 2158 (1976)

J.G.Cramer, R.M.DeVries, D.A.Goldberg, M.S.Zisman, C.F.Maguire

'Unique' Energy-Independent Woods-Saxon Optical Potential for 16O + 28Si Elastic Scattering

NUCLEAR REACTIONS 28Si(16O, 16O), E=215.2 MeV; measured σ(θ); deduced energy independent optical model parameters. Optical model analysis.

doi: 10.1103/PhysRevC.14.2158
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1976SH02      Phys.Rev. C13, 20 (1976)

J.D.Sherman, D.L.Hendrie, M.S.Zisman

Spectroscopy of the (α, 2α) Reaction at E = 90 MeV

NUCLEAR REACTIONS 12C, 16O, 24,26Mg, 28,30Si, 40,44Ca, 66Zn(α, 2α), E=90 MeV; measured σ(θ), αα(θ). 8Be, 12C, 20,22Ne, 24,26Mg, 36,40Ar, 62Ni levels deduced α-S. DWIA, PWIA analysis, α-cluster spectroscopy.

doi: 10.1103/PhysRevC.13.20
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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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1976VI02      Phys.Lett. 60B, 261 (1976)

D.J.Vieira, D.F.Sherman, M.S.Zisman, R.A.Gough, J.Cerny

Extension of the T(z) = -3/2 Beta-Delayed Proton Precursor Series to 57Zn

RADIOACTIVITY 53Ni(β+)[from 40Ca(16O, 3n)], 57Zn(β+)[from 40Ca (20Ne, 3n)]; measured β-delayed protons, Ep, T1/2. 53Co, 57Cu; deduced levels.

doi: 10.1016/0370-2693(76)90295-1
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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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1975BE11      Nucl.Phys. A242, 149 (1975)

M.Bernas, R.DeVries, B.G.Harvey, D.Hendrie, J.Mahoney, J.Sherman, J.Steyaert, M.S.Zisman

Anomaly in α-Scattering from 6Li between 35 and 45 MeV

NUCLEAR REACTIONS 6Li(α, α), (α, α'), E=34.75, 39.75, 45 MeV; measured angular distributions from 20° to 160° (cm), angular distributions analyzed with optical model, cut-off optical model, addition of the exchange contribution. Enriched target.

doi: 10.1016/0375-9474(75)90040-8
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1975ZI01      Phys.Rev. C11, 809 (1975)

M.S.Zisman, R.M.DeVries, J.G.Cramer, K.-L.Liu, Y.-d.Chan, B.Cuengco

16,18O Elastic Scattering from 58Ni

NUCLEAR REACTIONS 58Ni(18O, 18O), E=63.4 MeV; 58Ni(16O, 16O), E=63, 71.5, 81 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1103/PhysRevC.11.809
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1974BE58      Phys.Rev. C10, 1846 (1974)

F.D.Becchetti, B.G.Harvey, D.Kovar, J.Mahoney, M.S.Zisman

(16O, 15N) and (12C, 11B) Reactions on 54Fe and 62Ni at E(16O) = 104 MeV And E(12C) = 78 MeV

NUCLEAR REACTIONS 54Fe, 62Ni(16O, 15N), E=104 MeV; 54Fe, 62Ni(12C, 11B), E=78 MeV; measured σ(E(15N), θ), σ(E(11B), θ). 55Co, 63Cu levels deduced J, S.

doi: 10.1103/PhysRevC.10.1846
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1974DE03      Phys.Rev.Lett. 32, 680 (1974)

R.M.DeVries, M.S.Zisman, J.G.Cramer, K.-L.Liu, F.D.Becchetti, B.G.Harvey, H.Homeyer, D.G.Kovar, J.Mahoney, W.von Oertzen

Observation of an Anomalous Angular Distribution in the Single-Nucleon - Transfer Reaction 12C(14N, 13N)13C at 100 MeV

NUCLEAR REACTIONS 12C(14N, 13N), E=100 MeV; measured σ(E(13N), θ). 13C deduced levels, L.

doi: 10.1103/PhysRevLett.32.680
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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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1973ZI04      Phys.Rev. C8, 1866 (1973)

M.S.Zisman, F.D.Becchetti, B.G.Harvey, D.G.Kovar, J.Mahoney, J.D.Sherman

Heavy-Ion-Induced Single-Nucleon Transfer Reactions in the Zr-Mo Region

NUCLEAR REACTIONS 90,91,94Zr, 92Mo, 93Nb(16O, 15N), (16O, 15O), (16O, 16O'), E=104 MeV; 90Zr, 92Mo(12C, 11B), E=78 MeV; measured σ(E(15N), E(15O), E(11B), θ). 91,92,94,95Nb, 93Tc, 93,94Mo, 91,92,95Zr deduced levels, J, π, S, L.

doi: 10.1103/PhysRevC.8.1866
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1972BA14      Nucl.Phys. A181, 453 (1972)

A.D.Bacher, E.A.McClatchie, M.S.Zisman, T.A.Weaver, T.A.Tombrello

Observation of the 14 MeV Resonance in 12C(p, p)12C with Molecular Ion Beams

NUCLEAR REACTIONS 12C(p, p), E=14.2 MeV; measured σ(E), θ(lab)=165°. 13N deduced change in resonance shape of lowest T=3/2 level due to molecular ion beams.

doi: 10.1016/0375-9474(72)90495-2
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1972KO32      Phys.Rev.Lett. 29, 1023 (1972)

D.G.Kovar, F.D.Becchetti, B.G.Harvey, F.Puhlhofer, J.Mahoney, D.W.Miller, M.S.Zisman

j Dependence of Heavy-Ion-Induced Reactions

NUCLEAR REACTIONS 54Fe, 62Ni, 208Pb(16O, 15N), (12C, 11B), E=104, 78 MeV; measured σ ratios, σ(E(15N)), σ(E(11B)); deduced J-dependence. 55Co, 65Cu, 209Bi transitions deduced L.

doi: 10.1103/PhysRevLett.29.1023
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1972SH21      Phys.Rev. C6, 1082 (1972)

J.D.Sherman, B.G.Harvey, D.L.Hendrie, M.S.Zisman, B.Sorensen

Strong and Weak 0+ Excitations in the 142Ce(p, t)140Ce and 140Ce(p, t)138Ce Reactions

NUCLEAR REACTIONS 142Ce(p, t), 140Ce(p, t), E=30 MeV; measured σ(Et, θ). 138,140Ce deduced levels, L.

doi: 10.1103/PhysRevC.6.1082
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1972ZI01      Phys.Rev. C5, 1031 (1972)

M.S.Zisman, B.G.Harvey

High-Spin Levels of 92,93,94,95,96Nb and 94Tc Populated with (α, d) and (α, t) Reactions at 50 MeV

NUCLEAR REACTIONS 90,91,92,94Zr, 92Mo(α, d), 91,92,94Zr(α, t), E=50 MeV; measured σ(Ed, θ), σ(Et, θ). 92,93,95Nb, 94,96Nb, 94Tc deduced levels, configurations.

doi: 10.1103/PhysRevC.5.1031
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2756.


1971ZI03      Phys.Rev. C4, 1809 (1971)

M.S.Zisman, B.G.Harvey

High-Spin Proton States Observed in the Reactions 90Zr(α, t)91Nb and 92Mo(α, t)93Tc at 50 MeV

NUCLEAR REACTIONS 90Zr(α, t), 92Mo(α, t), E=50 MeV; measured σ(Et, θ), Q. 91Nb, 93Tc deduced levels, L(p), S.

doi: 10.1103/PhysRevC.4.1809
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2754.


1970ZI03      Phys.Rev. C2, 1271 (1970)

M.S.Zisman, E.A.McClatchie, B.G.Harvey

14N(α, d)16O Reaction at 40 MeV

NUCLEAR REACTIONS 14N(α, d), E=40 MeV; measured σ(Ed, θ). 16O deduced levels, level-width, T.

doi: 10.1103/PhysRevC.2.1271
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1969LU07      Phys.Rev. 186, 1086 (1969)

C.C.Lu, M.S.Zisman, B.G.Harvey

High-Spin States of Configuration (1d5/2)2(5+, 0) and (1g9/2)2(9+, 0) Strongly Populated by the (α, d) Reaction

NUCLEAR REACTIONS 13,14C, 15N, 20Ne(α, d), E = 40.1, 46, 45.4, 44.5 MeV; measured σ(Ed, θ). 15,16N, 17O, 22Na deduced levels, J, π, configuration. 52Cr, 54,56Fe, 58,60,62Ni, 64,66,68Zn(α, d), E = 50 MeV; measured σ(Ed, θ). 54Mn, 56,58Co, 60,62,64Cu, 66,68,70Ga deduced levels, J, π, configurations.

doi: 10.1103/PhysRev.186.1086
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0240.


1968LU04      UCRL-17989, p.61 (1968)

C.-C.Lu, M.S.Zisman, B.G.Harvey

High Spin Proton-Neutron Two-Particle Levels in the Medium-Mass (54 < a < 70) Region

NUCLEAR STRUCTURE 54Mn, 66Ga, 68Ga; measured not abstracted; deduced nuclear properties.


1968LU05      Phys.Lett. 27B, 217 (1968)

C.C.Lu, M.S.Zisman, B.G.Harvey

Proton-Neutron Two-Particle Excited States of the (1g9/2)2 9+ Configuration

NUCLEAR REACTIONS 52Cr, 54,56Fe, 58,60,62Ni, 64,66,68Zn(α, d), E=50 MeV; measured σ(Ed, θ). 54Mn, 56,58Co, 60,62,64Cu, 66,68,70Ga deduced level of (g9/2)2 configuration. Enriched targets.

doi: 10.1016/0370-2693(68)90276-1
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