NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = E.R.Cosman Found 38 matches. 1986OR01 Phys.Lett. 173B, 39 (1986) C.E.Ordonez, R.J.Ledoux, E.R.Cosman Rotational Band of 12C + 12C Gross-Structure Resonances and Its Representation by a Double-Minimum Optical Potential NUCLEAR REACTIONS, ICPND 12C(12C, 12C), E(cm)=5.5-33 MeV; analyzed reaction σ(E). 24Mg deduced shape isomeric doorway states. Double minimum optical potential.
doi: 10.1016/0370-2693(86)91226-8
1984AL25 Phys.Rev. C30, 1223 (1984) H.A.Aljuwair, R.J.Ledoux, M.Beckerman, S.B.Gazes, J.Wiggins, E.R.Cosman, R.R.Betts, S.Saini, O.Hansen Isotopic Effects in the Fusion of 40Ca with 40,44,48Ca NUCLEAR REACTIONS, ICPND 44,48,40Ca(40Ca, X), E=90-135 MeV; measured fusion σ(E). Velocity filter.
doi: 10.1103/PhysRevC.30.1223
1984LE19 Phys.Rev. C30, 866 (1984) R.J.Ledoux, C.E.Ordonez, M.J.Bechara, H.A.Al-Juwair, G.Lavelle, E.R.Cosman Selective Alpha Particle Decay of 12C + 12C Resonances to Excited 20Ne Rotational Bands Observed in the 12C(12C, α)20Ne Reaction NUCLEAR REACTIONS, ICPND 12C(12C, α), E(cm)=14-20.6 MeV; measured σ(Eα), σ(θ) vs E, yield vs E. 24Mg deduced resonances, J, π, Γα, reduced widths, possible isomeric resonance selective decay to 20Ne rotational band.
doi: 10.1103/PhysRevC.30.866
1983BE09 Phys.Rev. C27, 1540 (1983) M.J.Bechara, A.J.Lazzarini, R.J.Ledoux, E.R.Cosman 12C(16O, α)24Mg Reaction in the Energy Region E(c.m.) = 26.6 to 42.9 MeV NUCLEAR REACTIONS 12C(16O, α), E=62-100 MeV; measured σ(θ), σ(Eα), σ(θ, E). 24Mg deduced levels. 28Si deduced intermediate resonances, Γ, nonstatistical character.
doi: 10.1103/PhysRevC.27.1540
1983LA07 Phys.Rev. C27, 1550 (1983) A.J.Lazzarini, S.G.Steadman, R.J.Ledoux, A.Sperduto, G.R.Young, K.Van Bibber, E.R.Cosman Structure in the 12C + 12C and 8Be + 16O Fission Width Distribution of 24Mg Observed via the Reaction 12C(16O, α)24Mg → X + Y NUCLEAR REACTIONS, ICPND 12C(16O, α), E=77 MeV; measured σ(Eα), (α)(12C)(12C)-, (α)(8Be)(16O)-coin, summed three-body yields. 24Mg deduced resonances, Γ(12C)/Γ, three-body breakup characteristics. Cross correlation analysis.
doi: 10.1103/PhysRevC.27.1550
1983LE05 Phys.Rev. C27, 1103 (1983) R.J.Ledoux, M.J.Bechara, C.E.Ordonez, H.A.Al-Juwair, E.R.Cosman 12C + 12C Elastic Scattering Excitation Functions and Phase Shift Analysis NUCLEAR REACTIONS, ICPND 12C(12C, 12C), E(cm)=14.6-31.3 MeV; measured σ(θ) vs E; deduced reaction σ. 24Mg deduced intermediate resonances, J, π. Phase shift analysis.
doi: 10.1103/PhysRevC.27.1103
1980CO03 Phys.Rev. C21, 2111 (1980) E.R.Cosman, R.Ledoux, A.J.Lazzarini 12C + 12C Intermediate Structures Correlated among Elastic and Reaction Channels NUCLEAR REACTIONS 12C(12C, α), E(cm)=5-35 MeV; 12C(12C, p), 12C(12C, 12C'), E(cm)=16-23 MeV; 12C(12C, 12C), E=11-27 MeV; analyzed σ(E). 24Mg deduced intermediate structure resonances, Γ, Γα, Γ(12C) strength function, J, π. Cross correlation, Breit-Wigner analysis.
doi: 10.1103/PhysRevC.21.2111
1978LA05 Phys.Rev.Lett. 40, 1426 (1978) A.J.Lazzarini, E.R.Cosman, A.Sperduto, S.G.Steadman, W.Thoms, G.R.Young Population of Resonant 12C + 12C States via the Reaction 12C(16O, α)24Mg NUCLEAR REACTIONS 12C(16O, α), E=62-110 MeV; measured σ(E, Eα). 24Mg deduced levels.
doi: 10.1103/PhysRevLett.40.1426
1977CO02 Phys.Rev. C15, 654 (1977) T.M.Cormier, E.R.Cosman, A.J.Lazzarini, H.E.Wegner, J.D.Garrett, F.Puhlhofer Mass Systematics of Evaporation Residues from 35Cl- and 32S-Induced Fusion on Light Targets NUCLEAR REACTIONS 24,25,26Mg, 28Si, 27Al(32S, X), E=130 MeV; 28Si(28Si, X), E=117.5 MeV; 28Si, 24,25,26Mg(35Cl, X), E=145.6 MeV; 27Al(35Cl, X), E=100-170 MeV; measured fusion σ(A).
doi: 10.1103/PhysRevC.15.654
1976CO20 Phys.Rev. C14, 334 (1976) T.M.Cormier, E.R.Cosman, A.J.Lazzarini, J.D.Garrett, H.E.Wegner Two-Body Final-State Coincidence Measurements for Fissionlike Processes Following 35Cl + 27Al Fusion NUCLEAR REACTIONS 27Al(35Cl, X), E=170 MeV; measured fusion fragment-fragment (E, A).
doi: 10.1103/PhysRevC.14.334
1975CO10 Phys.Rev.Lett. 35, 265 (1975) E.R.Cosman, T.M.Cormier, K.Van Bibber, A.Sperduto, G.Young, J.Erskine, L.R.Greenwood, O.Hansen Evidence for a 12C + 12C Collective Band in 24Mg NUCLEAR REACTIONS 12C(12C, p), E(cm)=6.75-30 MeV; measured σ(E, Ep). 23Na deduced resonances, J, π. 24Mg deduced resonance anomaly.
doi: 10.1103/PhysRevLett.35.265
1975CO14 Nucl.Phys. A247, 377 (1975) T.M.Cormier, E.R.Cosman, L.Grodzins, O.Hansen, S.Steadman, K.Van Bibber, G.Young Gamma Rays from 23Na States Excited in the 12C(12C, p) Reaction at E = 38.6 MeV NUCLEAR REACTIONS 12C(12C, pγ), E=38.6 MeV; measured Eγ, Iγ, γγ-coin, pγ-coin. 23Na deduced levels, J, π.
doi: 10.1016/0375-9474(75)90643-0
1975DU08 Nucl.Phys. A247, 251 (1975) W.Dunnweber, E.R.Cosman, E.Grosse, W.R.Hering, P.Von Brentano Gamma Decay of Particle-Core States in 209Pb NUCLEAR REACTIONS 208Pb(d, pγ), E=11 MeV; measured Eγ, Iγ, pγ-coin. 209Pb deduced levels, J, π, B(λ).
doi: 10.1016/0375-9474(75)90635-1
1975GA12 Phys.Rev. C12, 481 (1975) J.D.Garrett, H.E.Wegner, T.M.Cormier, E.R.Cosman, A.J.Lazzarini Mass and Energy Distributions of Fusion Products from 32S on 12C, 25Mg, And 40Ca NUCLEAR REACTIONS 12C, 25Mg, 40Ca(32S, X), E=128.9 MeV; measured σ(E(fragment mass)).
doi: 10.1103/PhysRevC.12.481
1975GA13 Phys.Rev. C12, 489 (1975) J.D.Garrett, H.E.Wegner, T.M.Cormier, E.R.Cosman, O.Hansen, A.J.Lazzarini Elastic Scattering and Transfer Reactions Induced by 100 MeV 32S on 27Al NUCLEAR REACTIONS 27Al(32S, 32S), E=100 MeV; measured σ(θ). 27Al(32S, 31P), E=100 MeV; measured σ(E(31P), θ). 27Al(32S, 33S), E=100 MeV; measured σ(E(33S), θ). 27Al(32S, X), E=100 MeV; measured σ. 28Si levels deduced S.
doi: 10.1103/PhysRevC.12.489
1974CO17 Phys.Rev. C9, 2046 (1974) E.R.Cosman, A.Sperduto, T.M.Cormier, T.N.Chin, H.E.Wegner Comparison of the Structure Seen in the Reactions 16O(16O, α)28Si and 20Ne(12C, α)28Si NUCLEAR REACTIONS 16O(16O, α), E=35-70 MeV; 20Ne(12C, α), E=28-40 MeV; measured σ(E, Eα, θ).
doi: 10.1103/PhysRevC.9.2046
1974VA01 Phys.Rev.Lett. 32, 687 (1974) K.Van Bibber, E.R.Cosman, A.Sperduto, T.M.Cormier, T.N.Chin, O.Hansen Resonance in the Reaction 12C(12C, p)23Na at E(c.m.) = 19.3 MeV NUCLEAR REACTIONS 12C(12C, p), E(cm)=10-22 MeV; measured σ(E;Ep, θ). 23Na deduced levels. 24Mg deduced resonance, level-width.
doi: 10.1103/PhysRevLett.32.687
1973SL01 Nucl.Phys. A206, 433 (1973) D.C.Slater, E.R.Cosman, D.J.Pullen Particle Coupling to the Octupole State in 89Sr from 88Sr(p, p')88Sr Analog Resonances and 88Sr(d, p)89Sr NUCLEAR REACTIONS 88Sr(p, p'), Ep=7.65, 7.80, 7.92, 8.78, 9.75, 9.90 MeV, measured σ(E;θ). 89Y deduced isobaric analog resonances, Ip, J, π. 88Sr(d, p), Ed=10 MeV, measured σ(E, θ). 89Sr deduced L(n), S, J, π. Enriched target.
doi: 10.1016/0375-9474(73)90076-6
1973VO11 Nucl.Phys. A215, 61 (1973) P.B.Vold, J.O.Andreassen, J.R.Lien, A.Graue, E.R.Cosman, W.Dunnweber, D.Schmitt, F.Nusslin The 207Pb(d, p)208Pb Reaction with High Resolution NUCLEAR REACTIONS 207Pb(d, p), E=18 MeV; measured σ(Ep, θ). 208Pb deduced levels, L, J, π, spectroscopic strengths (2j+1)S. Enriched targets.
doi: 10.1016/0375-9474(73)90101-2
1972CO28 Phys.Rev.Lett. 29, 1341 (1972) E.R.Cosman, A.Sperduto, T.M.Cormier, T.N.Chin, H.E.Wegner, M.J.LeVine, D.Schwalm Structure in the Excitation Functions of 12C(16O, p)27Al, 12C(16O, d)26Al, and 12C(16O, α)24Mg NUCLEAR REACTIONS 12C(16O, p), (16O, d), (16O, α), E=10-26 MeV cms; measured σ(E); deduced large statistical compound-nucleus contribution. 28Si deduced resonance structure, level-width.
doi: 10.1103/PhysRevLett.29.1341
1972GR12 Nucl.Phys. A187, 141 (1972) A.Graue, L.H.Herland, K.J.Lervik, J.T.Nesse, E.R.Cosman The 90Zr(d, p)91Zr Reaction with High Resolution NUCLEAR REACTIONS 90Zr(d, p), E=7.5 MeV; measured σ(Ep, θ), Q; deduced transition strengths. 91Zr deduced levels, L(n), J, π, S.
doi: 10.1016/0375-9474(72)90079-6
1971CO24 Phys.Rev.Lett. 27, 1074 (1971) E.R.Cosman, A.Sperduto, W.H.Moore, T.N.Chin, T.M.Cormier Selective Population of Highly Excited States Seen in the Reaction 12C(16O, p)27Al NUCLEAR REACTIONS 12C(16O, p), E=36, 60 MeV; measured σ(Ep, θ). 27Al deduced selective population of 13-20 MeV states, yrast line.
doi: 10.1103/PhysRevLett.27.1074
1971GR04 Nucl.Phys. A162, 593 (1971) A.Graue, J.R.Lien, L.Rasmussen, G.E.Sandvik, E.R.Cosman The 31P(3He, p)33S Reaction NUCLEAR REACTIONS 31P(3He, p), E=12.0 MeV; measured σ(Ep, θ), Q. 33S deduced levels, L, J, π, isobaric analogs.
doi: 10.1016/0375-9474(71)90258-2
1971SP04 Phys.Rev. C3, 1179 (1971) J.E.Spencer, E.R.Cosman, H.A.Enge, A.K.Kerman Analysis of Proton Scattering and Reactions with the Generalized Optical Model NUCLEAR REACTIONS 88Sr(p, p), (p, p'), (p, n), E=4.8-8.2 MeV; measured nothing; deduced σ(E;θ). Generalized optical model. 89Sr; calculated levels, J, π.
doi: 10.1103/PhysRevC.3.1179
1970AN25 Nucl.Phys. A157, 561 (1970) T.R.Anfinsen, K.Bjorndal, A.Graue, J.R.Lien, G.E.Sandvik, L.O.Tveita, K.Ytterstad, E.R.Cosman Nuclear Reaction Studies in the Nickel Isotopes: The 62Ni(d, p)63Ni and 64Ni(d, p)65Ni Reactions NUCLEAR REACTIONS 62Ni(d, p), 64Ni(d, p), E=7.5 MeV; measured σ(Ep, θ), Q. 63Ni, 65Ni deduced levels, L(n), J, π, S. Enriched targets.
doi: 10.1016/0375-9474(70)90233-2
1970CO11 Phys.Rev. C1, 945 (1970) E.R.Cosman, R.Kalish, D.D.Armstrong, H.C.Britt Analog States of 89Sr and the Particle-Core Model in the N = 50 Region NUCLEAR REACTIONS 88Sr(p, p), (p, p'), E=4.8-12 MeV; measured σ(E;Ep'). 89Y deduced isobaric analog resonances, J, π.
doi: 10.1103/PhysRevC.1.945
1970SL01 Nucl.Phys. A147, 650 (1970) D.C.Slater, E.R.Cosman, J.E.Spencer Analogue States of 88Sr and the 87Sr(p, p)87Sr Reaction NUCLEAR REACTIONS 87Sr(p, p), (p, p'), Ep=4.5 to 7.5 MeV; measured σ(E;θ). 88Y deduced isobaric analog resonances, L(p), level-width, p-width, S. Enriched target.
doi: 10.1016/0375-9474(70)90606-8
1969CO07 Phys.Rev. 182, 1131 (1969) E.R.Cosman, D.C.Slater, J.E.Spencer Isobaric Analog States of Ti51 Studied by Elastic and Inelastic Scattering of Protons on Ti50 NUCLEAR REACTIONS 50Ti(p, p), (p, p'), E=3.4-7.2 MeV; measured σ(E;θ). 51V deduced resonances, level-width. Isobaric analog.
doi: 10.1103/PhysRev.182.1131
1969GR23 Nucl.Phys. A136, 577 (1969) A.Graue, L.H.Herland, J.R.Lien, G.E.Sandvik, E.R.Cosman, W.H.Moore A Study of the 35Cl Levels by Means of the 34S(3He, d)35Cl Reaction NUCLEAR REACTIONS 34S(3He, d), E = 11.0 MeV; measured σ(Ed, θ), Q; deduced transition strengths. 35Cl deduced levels, S, L(p), isospin, analog states.
doi: 10.1016/0375-9474(69)90129-8
1968CO01 Nucl.Phys. A109, 305 (1968) E.R.Cosman, D.N.Schramm, H.A.Enge A Study of 61Ni by the 59Co(3He, P)61Ni Reaction NUCLEAR REACTIONS 59Co(3He, p), E=11.65 MeV, measured (Ep, θ); deduced Q. 61Ni deduced levels. Enriched target.
doi: 10.1016/0375-9474(68)90595-2
1968CO02 Nucl.Phys. A108, 519 (1968) E.R.Cosman, J.M.Joyce, S.M.Shafroth A Study of the Low-Lying Isobaric Analogue States of 89Sr by Means of the 88Sr(p, p) and (p, p') Reactions NUCLEAR REACTIONS 88Sr(p, p), (p, p'), E = 5.0 to 8.7 MeV; measured σ(E; Ep', θ). 89Y deduced analog levels, L(p), level-width. Enriched target.
doi: 10.1016/0375-9474(68)90320-5
1968CO03 Phys.Rev. 165, 1175 (1968) E.R.Cosman, H.A.Enge, A.Sperduto Nuclear-Reaction Studies in the Strontium Isotopes: The Sr88(d, p)Sr89 Reaction NUCLEAR STRUCTURE 89Sr; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.165.1175
1968CO20 Phys.Rev. 172, 1126 (1968) Nuclear-Reaction Studies in the Strontium Isotopes: Neutron Particle-Hole States in Sr88 and Sr87(d, p)Sr88 Reaction NUCLEAR REACTIONS 87Sr(d, p), E=7.5 MeV; measured σ(Ep, θ). 88Sr deduced levels, J, π.
doi: 10.1103/PhysRev.172.1126
1968GR17 Nucl.Phys. A120, 513 (1968) A.Graue, L.Herland, J.R.Lien, E.R.Cosman A Study of the 32S Levels and the Analogue Levels of 32P by the 31P(3He, d)32S Reaction NUCLEAR REACTIONS 31P(3He, d), E=12.0 MeV; measured σ(Ed, θ), Q; deduced transition strengths. 32S deduced levels, L(p), isospin, analog states.
doi: 10.1016/0375-9474(68)90458-2
1967CO27 Phys.Rev. 163, 1134 (1967) E.R.Cosman, D.N.Schramm, H.A.Enge, A.Sperduto, C.H.Paris Nuclear-Reaction Studies in the Nickel Isotopes: The Ni61(p, p')Ni61, Ni61(d, d')Ni61, and Ni60(d, p)Ni61 NUCLEAR STRUCTURE 61Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.1134
1966CO11 Phys.Rev. 142, 673 (1966) E.R.Cosman, C.H.Paris, A.Sperduto, H.A.Enge Nuclear-Reaction Studies in the Nickel Isotopes: The Ni58(p, p')Ni58 and Ni58(d, p)Ni59 Reactions NUCLEAR STRUCTURE 59Ni, 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.142.673
1966CO20 Phys.Lett. 22, 195 (1966) E.R.Cosman, H.A.Enge, A.Sperduto Study of Low-Lying Isobaric Analogue States of 89Sr NUCLEAR STRUCTURE 89Y, 89Sr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90572-5
1966CO33 Bull.Am.Phys.Soc. 11, No.3, 318, BB5 (1966); and Priv.Comm. E.R.Cosman, A.Sperduto, H.A.Enge Energy Levels of Ni61 from the (p, p'), (d, d'), and (d, p) Reactions NUCLEAR STRUCTURE 61Ni; measured not abstracted; deduced nuclear properties.
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