NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.S.Zisman Found 61 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1972ZI01 Phys.Rev. C5, 1031 (1972) 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
1971ZI03 Phys.Rev. C4, 1809 (1971) 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
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
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
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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