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NSR database version of April 11, 2024.

Search: Author = D.G.Kovar

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1994VI01      Phys.Rev. C49, 948 (1994)

M.F.Vineyard, S.E.Atencio, J.F.Crum, G.P.Gilfoyle, B.G.Glagola, D.J.Henderson, D.G.Kovar, C.F.Maguire, J.F.Mateja, R.G.Ohl, F.W.Prosser, J.H.Rollinson, R.S.Trotter

Light-Particle Correlations with Evaporation Residues in the 40Ca + 12C Reaction at E(40Ca) = 450 MeV

NUCLEAR REACTIONS 12C(40Ca, X), E=450 MeV; measured α(evaporation residue)-, p(evaporation residue)-coin, α-multiplicity vs θα, Eα, p-multiplicity vs θp, Ep; deduced pre-equilibrium α-, p-emission. Statistical model.

doi: 10.1103/PhysRevC.49.948
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1993VI02      Phys.Rev. C47, 2374 (1993)

M.F.Vineyard, J.F.Mateja, C.Beck, S.E.Atencio, L.C.Dennis, A.D.Frawley, D.J.Henderson, R.V.J.Janssens, K.W.Kemper, D.G.Kovar, C.F.Maguire, S.J.Padalino, F.W.Prosser, G.S.F.Stephans, M.A.Tiede, B.D.Wilkins, R.A.Zingarelli

Energy Dependence of Fusion Evaporation-Residue Cross Sections in the 28Si + 12C Reaction

NUCLEAR REACTIONS 12C(28Si, X), E(cm)=18-136 MeV; measured σ(evaporation residue) vs E, fragment velocity distributions. Model comparison. Other reactions analyzed.

doi: 10.1103/PhysRevC.47.2374
Citations: PlumX Metrics

1992GI03      Phys.Rev. C46, 265 (1992)

G.P.Gilfoyle, M.S.Gordon, R.L.McGrath, G.Auger, J.M.Alexander, D.G.Kovar, M.F.Vineyard, C.Beck, D.J.Henderson, P.A.DeYoung, D.Kortering

Heavy Residue Production in 215 MeV 16O + 27Al Reactions

NUCLEAR REACTIONS 27Al(16O, X), E=215 MeV; measured (particle)(particle)-coin, fragment mass, velocity distributions; deduced evidence for heavy fragment production.

doi: 10.1103/PhysRevC.46.265
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1992VI01      Phys.Rev. C45, 1784 (1992)

M.F.Vineyard, J.S.Bauer, J.F.Crum, C.H.Gosdin, R.S.Trotter, D.G.Kovar, C.Beck, D.J.Henderson, R.V.F.Janssens, B.D.Wilkins, C.F.Maguire, J.F.Mateja, F.W.Prosser, G.S.F.Stephans

Fusion Evaporation-Residue Cross Sections for 28Si + 40Ca at E(28Si) = 309, 397, and 452 MeV

NUCLEAR REACTIONS 40Ca(28Si, X), E=309-452 MeV; measured σ(evaporation residue θ); deduced entrance channel mass-asymmetry role. Model comparison.

doi: 10.1103/PhysRevC.45.1784
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1990DE11      Phys.Rev. C41, R1885 (1990)

P.A.DeYoung, C.J.Gelderloos, D.Kortering, J.Sarafa, K.Zienert, M.S.Gordon, B.J.Fineman, G.P.Gilfoyle, X.Lu, R.L.McGrath, D.M.de Castro Rizzo, J.M.Alexander, G.Auger, S.Kox, L.C.Vaz, C.Beck, D.J.Henderson, D.G.Kovar, M.F.Vineyard

Particle-Particle Correlations and Lifetimes of Composite Nuclei: New tests for the evaporation model and for statistical equilibration

NUCLEAR REACTIONS 27Al(16O, 2p), (16O, pd), E=80-250 MeV; measured pp-, pd-correlations; deduced evaporative decay T1/2. Statistical model.

doi: 10.1103/PhysRevC.41.R1885
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1990KR14      Phys.Rev.Lett. 65, 2118 (1990)

R.A.Kryger, J.J.Kolata, W.Chung, S.Dixit, R.J.Tighe, J.J.Vega, P.A.De Young, C.Copi, J.Sarafa, D.G.Kovar, G.P.Gilfoyle, S.K.Sigworth

Two-Particle Correlations from Neutron-Light-Charged-Particle Coincidences

NUCLEAR REACTIONS 27Al(16O, nX), E=215 MeV; measured nX-coin for X=α, d, p; deduced singlet-d, 5He production evidence. 43Sc deduced nuclear temperature.

doi: 10.1103/PhysRevLett.65.2118
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1990RE13      Phys.Rev. C42, 2497 (1990); Erratum Phys.Rev. C44, 1717 (1991)

K.E.Rehm, C.Beck, A.van den Berg, D.G.Kovar, L.L.Lee, W.C.Ma, F.Videbaek, T.F.Wang

Systematic Behavior of One- and Two-Nucleon Transfer Reactions Induced by Medium-Weight Projectiles

NUCLEAR REACTIONS, ICPND 208Pb(80Se, 81Se), (80Se, 82Se), E=525 MeV; 208Pb(64Ni, 65Ni), (64Ni, 66Ni), E=380 MeV; measured σ(θ); calculated reaction σ. DWBA analysis.

doi: 10.1103/PhysRevC.42.2497
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1990SA14      Phys.Rev. C41, R1901 (1990)

S.J.Sanders, B.B.Back, R.V.F.Janssens, D.G.Kovar, D.Habs, D.Henderson, T.-L.Khoo, H.Korner, G.-E.Rathke, T.F.Wang, F.L.H.Wolfs, K.B.Beard

Additional Evidence for Fusion-Fission in 32S + 24Mg Reactions: Division of excitation energy and spin in the fission fragments

NUCLEAR REACTIONS 24Mg(32S, 12C), E=140 MeV; measured γ(12C)-coin, E(γ); deduced reaction mechanism, scission temperature.

doi: 10.1103/PhysRevC.41.R1901
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1990VI01      Phys.Rev. C41, 1005 (1990)

M.F.Vineyard, J.S.Bauer, C.H.Gosdin, R.S.Trotter, D.G.Kovar, C.Beck, D.J.Henderson, R.V.F.Janssens, B.D.Wilkins, G.Rosner, P.Chowdhury, H.Ikezoe, W.Kuhn, J.J.Kolata, J.D.Hinnefeld, C.F.Maguire, J.F.Mateja, F.W.Prosser, G.S.F.Stephans

Energy Dependence of Fusion Evaporation-Residue Cross Sections in the 28Si + 28Si Reaction

NUCLEAR REACTIONS, ICPND 28Si(28Si, X), E=174-452 MeV; measured σ(E, θ); deduced critical angular momenta, fusion σ(E). Fusion evaporation residues, complete, incomplete fusion.

doi: 10.1103/PhysRevC.41.1005
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1989BE17      Phys.Rev. C39, 2202 (1989)

C.Beck, D.G.Kovar, S.J.Sanders, B.D.Wilkins, D.J.Henderson, R.V.F.Janssens, W.C.Ma, M.F.Vineyard, T.F.Wang, C.F.Maguire, F.W.Prosser, G.Rosner

Fusion of 16O + 40Ca at E(lab)(16O) = 13.4 MeV/Nucleon

NUCLEAR REACTIONS 40Ca(16O, X), E=13.4 MeV/nucleon; measured evaporation residue σ(θ), fusion-fission fragment σ(θ); deduced fusion σ(E) limits.

doi: 10.1103/PhysRevC.39.2202
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1989PR05      Phys.Rev. C40, 2600 (1989)

F.W.Prosser, S.V.Reinert, D.G.Kovar, G.Rosner, G.S.F.Stephans, J.J.Kolata, C.F.Maguire, A.Szanto de Toledo, E.Szanto

Fusion-Evaporation Cross Sections for 24Mg + 24Mg at 5 < E(lab) < 9 MeV/Nucleon

NUCLEAR REACTIONS 24Mg(24Mg, 24Mg), (24Mg, X), E=111, 160, 206 MeV; measured evaporation residue σ(E, mass, θ), elastic σ(θ); deduced Galilean-invariant velocity distributions, limits on incomplete fusion. Model comparisons.

doi: 10.1103/PhysRevC.40.2600
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1989SA39      Phys.Rev. C40, 2091 (1989)

S.J.Sanders, D.G.Kovar, B.B.Back, C.Beck, D.J.Henderson, R.V.F.Janssens, T.F.Wang, B.D.Wilkins

Binary Decay of 56Ni Formed in the 32S + 24Mg Reaction

NUCLEAR REACTIONS 24Mg(32S, X), E=120.4, 141.2 MeV; measured σ(fragment mass, E, θ); deduced fusion-fission σ. Binary decay, coincidence geometry.

doi: 10.1103/PhysRevC.40.2091
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1989VO02      Phys.Rev. C39, 1377 (1989)

R.J.Vojtech, J.J.Kolata, L.A.Lewandowski, K.E.Rehm, D.G.Kovar, G.S.F.Stephans, M.F.Vineyard

Quasielastic Scattering of 30Si on 208Pb and the Quadrupole Moments of 2+ Levels in 30Si

NUCLEAR REACTIONS 208Pb(30Si, 30Si), (30Si, 30Si'), (30Si, 31Si), (30Si, 29Al), E=222 MeV; measured σ(θ); deduced optical model parameters; inelastic interference terms. 30Si levels deduced static quadrupole moment.

doi: 10.1103/PhysRevC.39.1377
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1988RE07      Phys.Rev. C37, 2629 (1988)

K.E.Rehm, A.M.van den Berg, J.J.Kolata, D.G.Kovar, W.Kutschera, G.Rosner, G.S.F.Stephans, J.L.Yntema

Transition from Quasi-Elastic to Deep-Inelastic Reactions in the 48Ti + 208Pb System

NUCLEAR REACTIONS 208Pb(46Ti, 45Ti), (46Ti, 48Ti), (46Ti, 47Ti), (48Ti, 49Ti), (48Ti, 50Ti), (48Ti, 47Ti), (48Ti, 51Ti), (50Ti, 51Ti), (50Ti, 52Ti), (50Ti, 49Ti), E=298-300 MeV; measured σ(θ); deduced σ, Wilczynski plots, Q, quasielastic σ.

doi: 10.1103/PhysRevC.37.2629
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1988TS01      Phys.Rev.Lett. 60, 14 (1988)

I.Tserruya, V.Steiner, Z.Fraenkel, P.Jacobs, D.G.Kovar, W.Henning, M.F.Vineyard, B.G.Glagola

Incomplete Fusion Reactions Induced by 12C at 5.5-10 MeV/Nucleon

NUCLEAR REACTIONS, ICPND 120Sn, 160Gd, 197Au(12C, X), E=5.5-10 MeV/nucleon; measured complete, incomplete fusion σ(E), σ(θ).

doi: 10.1103/PhysRevLett.60.14
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1987HI10      Phys.Rev. C36, 989 (1987)

J.D.Hinnefeld, J.J.Kolata, D.J.Henderson, R.V.F.Janssens, D.G.Kovar, K.T.Lesko, G.Rosner, G.S.F.Stephans, A.M.Van Den Berg, B.D.Wilkins, F.W.Prosser, S.V.Reinert, P.L.Gonthier

Velocity and Angular Distributions of Evaporation Residues from 32S-Induced Reactions

NUCLEAR REACTIONS 12C, 24Mg, 27Al, 28Si, 40Ca(32S, X), E=194, 239, 278 MeV; measured evaporation residue spectra, σ(fragment θ). 24Mg(32S, 32S), E=194, 239, 278 MeV; measured σ(θ); deduced σ(E), complete fusion limitations.

doi: 10.1103/PhysRevC.36.989
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1987SA52      Phys.Rev.Lett. 59, 2856 (1987)

S.J.Sanders, D.G.Kovar, B.B.Back, C.Beck, B.K.Dichter, D.Henderson, R.V.F.Janssens, J.G.Keller, S.Kaufman, T.-F.Wang, B.Wilkins, F.Videbaek

Asymmetric Fission of 56Ni

NUCLEAR REACTIONS, ICPND 24Mg(32S, X), E=141.8 MeV; measured mass, velocity spectra, binary reaction σ(A); deduced fission reaction yield characteristics. 56Ni deduced fission mechanism.

doi: 10.1103/PhysRevLett.59.2856
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1987ST01      Phys.Rev. C35, 614 (1987)

G.S.F.Stephans, R.V.F.Janssens, D.G.Kovar, B.D.Wilkins

Projectilelike Fragments from 14N Beams at 15, 25, and 35 MeV/Nucleon

NUCLEAR REACTIONS 12C, 24Mg, 27Al, 48Ti, 58Ni(14N, X), E=15, 25, 35 MeV/nucleon; measured fragment momentum distributions for X=4He, 6,7Li, 7Be, 10,11B, 11,12,13C, 13,15N, 15O; deduced momentum widths, centroids. ΔE-E telescope.

doi: 10.1103/PhysRevC.35.614
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1987VA22      Phys.Lett. 194B, 334 (1987)

A.M.Van den Berg, K.E.Rehm, D.G.Kovar, W.Kutschera, G.S.F.Stephans

Systematics of Quasi-Elastic Neutron Transfer Cross Sections for Heavy-Ion Induced Reactions

NUCLEAR REACTIONS 144,149,154Sm(58Ni, 58Ni), (58Ni, 58Ni'), (58Ni, 57Ni), (58Ni, 59Ni), (58Ni, 60Ni), E=245 MeV; measured σ, σ(θ); deduced target mass dependence, quasielastic transfer systematics. Enriched targets. DWBA calculations.

doi: 10.1016/0370-2693(87)91060-4
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1987VO04      Phys.Rev. C35, 2139 (1987)

R.J.Vojtech, J.J.Kolata, L.A.Lewandowski, K.E.Rehm, D.G.Kovar, G.S.F.Stephans, G.Rosner, H.Ikezoe, M.F.Vineyard

Quasielastic Processes in the 28Si + 208Pb Reaction at 6 MeV/nucleon

NUCLEAR REACTIONS 208Pb(28Si, 28Si), (28Si, 28Si'), (28Si, X), E=166 MeV; measured σ(θ), σ(fragment E) for X=27Al, 29,30,31Si; deduced inelastic, reaction, transfer σ, ratios. Enriched target. DWBA calculations.

doi: 10.1103/PhysRevC.35.2139
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1986VI02      Phys.Rev. C33, 1325 (1986)

M.F.Vineyard, D.G.Kovar, G.S.F.Stephans, K.E.Rehm, G.Rosner, H.Ikezoe, J.J.Kolata, R.Vojtech

Quasi-Elastic Processes in the 28Si + 40Ca Reaction at 225 MeV

NUCLEAR REACTIONS 40Ca(28Si, 28Si), (28Si, 28Si'), (28Si, 27Al), (28Si, 27Si), (28Si, 29Si), E=225 MeV; measured particle spectra, σ(θ); deduced transfer reaction total spectroscopic factors, σ. 40Ca, 28Si transition deduced deformation lengths. 41Sc, 39,41Ca levels deduced spectroscopic factors. Optical model, DWBA analyses.

doi: 10.1103/PhysRevC.33.1325
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1985MA10      Phys.Rev. C31, 867 (1985)

J.F.Mateja, A.D.Frawley, D.G.Kovar, D.Henderson, H.Ikezoe, R.V.F.Janssens, G.Rosner, G.S.F.Stephans, B.Wilkins, K.T.Lesko, M.F.Vineyard

10B + 13C and 11B + 12C Reactions from 4 to 9 MeV/Nucleon

NUCLEAR REACTIONS, ICPND 12C(11B, X), (11B, 11B), 13C(10B, 10B), (10B, X), E=4-9 MeV/nucleon; measured σ(θ), σ(fragment E) for fragment mass=15, 20, 11, 6, fusion σ vs E; deduced nonfusion σ for mass 6-13, entrance channel role in fusion. 23Na deduced critical L vs excitation energy.

doi: 10.1103/PhysRevC.31.867
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1985SA11      Phys.Rev. C31, 1775 (1985)

S.J.Sanders, H.Ernst, W.Henning, C.Jachcinski, D.G.Kovar, J.P.Schiffer, J.Barrette

Energy Dependence of the Cross Sections for the 24Mg(16O, 12C)28Si(g.s) Reaction

NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=36-54 MeV; measured σ(E), σ(θ). 40Ca deduced possible resonances, parameters.

doi: 10.1103/PhysRevC.31.1775
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1985ST20      Phys.Lett. 161B, 60 (1985)

G.S.F.Stephans, D.G.Kovar, R.V.F.Janssens, G.Rosner, H.Ikezoe, B.Wilkins, D.Henderson, K.T.Lesko, J.J.Kolata, C.K.Gelbke, B.V.Jacak, Z.M.Koenig, G.D.Westfall, A.Szanto De Toledo, E.M.Szanto, P.L.Gonthier

Influence of Nucleon Fermi Motion on Incomplete Fusion

NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 40Ca, 48Ti(14N, X), E=5-35 MeV/nucleon; measured evaporation residue velocity spectra; deduced Fermi motion role in inelastic fusion. Other data input.

doi: 10.1016/0370-2693(85)90609-4
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1984KO14      Phys.Rev. C30, 125 (1984)

J.J.Kolata, K.E.Rehm, D.G.Kovar, G.S.F.Stephans, G.Rosner, H.Ikezoe, R.Vojtech

Quasielastic Processes in the 28Si + 208Pb Reaction at 8 MeV per Nucleon

NUCLEAR REACTIONS 208Pb(28Si, 28Si), (28Si, 28Si'), (28Si, 29Si), (28Si, 30Si), (28Si, 27Al), E=225 MeV; measured σ(θ), quasielastic yields, optimum Q, σ(E(28Si)), σ(E(29Si)), σ(E(30Si)). 208Pb(28Si, 27Si), (28Si, 31Si), (28Si, 25Al), (28Si, 26Al), (28Si, 28Al), (28Si, 29Al), (28Si, 27Mg), (28Si, 26Mg), (28Si, 25Mg), (28Si, 24Mg), (28Si, 23Mg), E=225 MeV; measured mass spectra; deduced optical model potentials. 28Si levels deduced deformation parameters, electromagnetic transition matrix elements. 208Pb levels deduced deformation lengths, electromagnetic transition matrix elements.

doi: 10.1103/PhysRevC.30.125
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1983PE08      Phys.Rev. C28, 710 (1983)

J.F.Petersen, R.J.Ascuitto, D.G.Kovar, W.Henning, S.J.Sanders

12C on 48Ca Transfer Reactions: A test of the effective Q-value model

NUCLEAR REACTIONS 48Ca(12C, 11B), (12C, 13C), (12C, 12C), E=45 MeV; measured σ(θ), σ(E(11B)), σ(E(13C)); deduced optical model parameters. DWBA, effective Q model analyses.

doi: 10.1103/PhysRevC.28.710
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1983RE08      Phys.Rev.Lett. 51, 1426 (1983)

K.E.Rehm, D.G.Kovar, W.Kutschera, M.Paul, G.Stephans, J.L.Yntema

Large Cross Sections for Quasielastic Neutron-Pickup Reactions Induced by 37Cl, 48Ti, and 58Ni on 208Pb

NUCLEAR REACTIONS 208Pb(58Ni, 59Ni), (58Ni, 60Ni), (58Ni, X), (37Cl, X), (48Ti, X), E=250, 300, 375 MeV; measured quasielastic yields, σ(fragment A), σ(E(59Ni)), σ(E(60Ni)), σ(θ(59Ni)), σ(θ(60Ni)); deduced σ(reaction), neutron pickup σ contributions. DWBA analysis.

doi: 10.1103/PhysRevLett.51.1426
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1982DA09      Phys.Rev. C25, 1342 (1982)

K.Daneshvar, D.G.Kovar, S.J.Krieger, K.T.R.Davies

Fusion Cross Section Behavior for 12C + 24Mg and 12C + 26Mg

NUCLEAR REACTIONS, ICPND 24Mg(12C, X), E=20-63 MeV; measured fusion σ(E). 24Mg(12C, 12C), (12C, X), E=20-60 MeV; 26Mg(12C, 12C), (12C, X), E=20-56 MeV; measured elastic σ, fusion σ vs θ. Macroscopic, microscopic fusion models.

doi: 10.1103/PhysRevC.25.1342
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1982MO15      Phys.Lett. 113B, 463 (1982)

H.Morgenstern, W.Bohne, K.Grabisch, D.G.Kovar, H.Lehr

Incomplete Momentum Transfer in Heavy-Ion Fusion at 14.5 MeV/Nucleon

NUCLEAR REACTIONS 12C, 27Al, 40Ca(20Ne, X)32S/47V/60Zn, E=291 MeV; measured σ (fragment θ) vs velocity; deduced incomplete momentum transfer in fusion.

doi: 10.1016/0370-2693(82)90786-9
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1982RA25      Phys.Rev. C26, 2022 (1982)

R.A.Racca, F.W.Prosser, C.N.Davids, D.G.Kovar

Search for Structure in the Fusion of 16O + 24Mg

NUCLEAR REACTIONS, ICPND 24Mg(16O, 2p), (16O, np), (16O, pα), (16O, 2α), (16O, 2pα), (16O, p2α), E=40-51 MeV; measured residuals production σ(E); deduced no structure in fusion σ vs E. Activation technique.

doi: 10.1103/PhysRevC.26.2022
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1982RE03      Phys.Rev. C25, 1915 (1982)

K.E.Rehm, W.Henning, J.R.Erskine, D.G.Kovar, M.H.Macfarlane, S.C.Pieper, M.Rhoades-Brown

Inelastic Scattering of 16O from 40,42,44,48Ca

NUCLEAR REACTIONS 40,42,44Ca(16O, 16O), (16O, 16O'), E=60 MeV; 48Ca(16O, 16O), (16O, 16O'), E=56 MeV; measured σ(θ), σ(E(16O)). 40Ca levels deduced deformation lengths. 42,44,48Ca levels deduced deformation lengths, B(λ). DWBA, coupled-channels analysis.

doi: 10.1103/PhysRevC.25.1915
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1982RE14      Phys.Rev. C26, 1010 (1982)

K.E.Rehm, W.Henning, J.R.Erskine, D.G.Kovar

Inelastic Scattering and One-Neutron-Transfer Reactions of 18O + 40Ca

NUCLEAR REACTIONS 40Ca(18O, 18O), (18O, 18O'), (18O, 17O), (18O, 19F), E=62.14 MeV; measured σ(θ), σ(E(17O)), σ(E(19F)). 18O, 40Ca transition deduced deformation lengths. 41Ca levels deduced spectroscopic factors. Optical model, DWBA, coupled-channels calculations.

doi: 10.1103/PhysRevC.26.1010
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1981JA10      Phys.Rev. C24, 2070 (1981)

C.M.Jachcinski, D.G.Kovar, R.R.Betts, C.N.Davids, D.F.Geesaman, C.Olmer, M.Paul, S.J.Sanders, J.L.Yntema

Fusion of 24Mg + 24Mg

NUCLEAR REACTIONS 24Mg(24Mg, X), E(cm)=24.7-66.2 MeV; measured σ(fusion, E). Activation technique.

doi: 10.1103/PhysRevC.24.2070
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1981TA16      Phys.Rev. C24, 960 (1981)

S.L.Tabor, L.C.Dennis, K.W.Kemper, J.D.Fox, K.Abdo, G.Neuschaefer, D.G.Kovar, H.Ernst

Fragmentation of 16O and 18O Projectiles

NUCLEAR REACTIONS 12C, 27Al, 46Ti(16O, X), (18O, X), E=72, 141 MeV; measured σ(fragment E, θ), σ(θ) for Li, Be, B, C, N; deduced projectile fragmentation vs E. Simple breakup model.

doi: 10.1103/PhysRevC.24.960
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1980PA08      Phys.Rev. C21, 1802 (1980)

M.Paul, S.J.Sanders, D.F.Geesaman, W.Henning, D.G.Kovar, C.Olmer, J.P.Schiffer, J.Barrette, M.J.LeVine

24Mg(16O, 12C)28Si and 24Mg(16O, 16O)24Mg Reactions at Backward Angles

NUCLEAR REACTIONS 24Mg(16O, 12C), (16O, 16O), E=24-40 MeV; measured σ(E, θ). 40Ca deduced resonances, J. DWBA, Legendre polynomial, correlation analyses.

doi: 10.1103/PhysRevC.21.1802
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1980PR06      Phys.Rev. C21, 1819 (1980)

F.W.Prosser, Jr., R.A.Racca, K.Daneshvar, D.F.Geesaman, W.Henning, D.G.Kovar, K.E.Rehm, S.L.Tabor

Complete Fusion of 15N + 27Al

NUCLEAR REACTIONS 27Al(15N, 15N), (15N, X), E=27-70 MeV; measured fusion σ(E), elastic σ(θ); deduced entrance channel effects. Glas-Mosel, Horn-Ferguson models.

doi: 10.1103/PhysRevC.21.1819
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1980SA12      Phys.Rev. C21, 1810 (1980)

S.J.Sanders, M.Paul, J.Cseh, D.F.Geesaman, W.Henning, D.G.Kovar, R.Kozub, C.Olmer, J.P.Schiffer

Resonant Behavior of the 24Mg(16O, 12C)28Si Reaction

NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=26.3-32.4 MeV; measured σ(E, θ). 40Ca deduced resonances, J, Γ. Breit-Wigner resonance, direct amplitudes.

doi: 10.1103/PhysRevC.21.1810
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1980SA31      Phys.Rev. C22, 1914 (1980)

S.J.Sanders, C.Olmer, D.F.Geesaman, W.Henning, D.G.Kovar, M.Paul, J.P.Schiffer

Resonant Behavior of the 24Mg(16O, 12C)28Si* (6.4 < Ex < 10 MeV) Reaction

NUCLEAR REACTIONS 24Mg(16O, 12C), E(cm)=24-36 MeV; measured σ(E, θ), σ(E(12C)). 40Ca resonances deduced entrance, exit channel partial widths. DWBA analysis.

doi: 10.1103/PhysRevC.22.1914
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1979KO20      Phys.Rev. C20, 1305 (1979)

D.G.Kovar, D.F.Geesaman, T.H.Braid, Y.Eisen, W.Henning, T.R.Ophel, M.Paul, K.E.Rehm, S.J.Sanders, P.Sperr, J.P.Schiffer, S.L.Tabor, S.Vigdor, B.Zeidman, F.W.Prosser, Jr.

Systematics of Carbon- and Oxygen-Induced Fusion on Nuclei with 12 ≤ A ≤ 19

NUCLEAR REACTIONS 12C(12C, X), E(cm)=7.4-31.2 MeV; 12C(13C, X), E(cm)=7.6-24.9 MeV; 12C(14N, X), E(cm)=15.1-24.0 MeV; 12C(15N, X), E(cm)=8.9-26.7 MeV; 12C(16O, X), E(cm)=12.9-27.0 MeV; 12C(18O, X), E(cm)=11.9-28.0 MeV; 12C(19F, X), E(cm)=11.6-27.1 MeV; 16O(16O, X), E(cm)=16.9-36.0 MeV; measured fusion σ(E); deduced fusion barrier parameters.

doi: 10.1103/PhysRevC.20.1305
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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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1978GE09      Phys.Rev. C18, 284 (1978)

D.F.Geesaman, C.N.Davids, W.Henning, D.G.Kovar, K.E.Rehm, J.P.Schiffer, S.L.Tabor, F.W.Prosser, Jr.

Search for Structure in the Fusion of 16O + 40Ca

NUCLEAR REACTIONS 40Ca(16O, X), E=45-63 MeV; measured fusion σ(E).

doi: 10.1103/PhysRevC.18.284
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1978HE14      Phys.Rev. C17, 2245 (1978)

W.Henning, Y.Eisen, H.-J.Korner, D.G.Kovar, J.P.Schiffer, S.Vigdor, B.Zeidman

Optimum Q Value in Heavy-Ion-Induced Neutron Transfer at the Coulomb Barrier

NUCLEAR REACTIONS 118Sn(18O, 16O), E=53-62 MeV; measured σ(E, θ); deduced optimum Q.

doi: 10.1103/PhysRevC.17.2245
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1978JA19      Phys.Rev. C18, 2656 (1978)

H.E.Jackson, S.B.Kaufman, D.G.Kovar, L.Meyer-Schutzmeister, K.E.Rehm, J.P.Schiffer, S.L.Tabor, S.E.Vigdor, T.P.Wangler, L.L.Rutledge, Jr., R.E.Segel, R.L.Burman, P.A.M.Gram, R.P.Redwine, M.A.Yates-Williams

Gamma-Ray Study of Pion-Induced Reactions on the Nickel Isotopes

NUCLEAR REACTIONS 58,60,62,64Ni(π+, Xγ), E=100, 160, 220 MeV; measured prompt, β-delayed γ-spectra. 57,58,59,60,61,62,64Ni, 57,59,60,61Co, 54,55,56,58Fe, 53,55Mn, 50,51,52Cr, 49,51V, 45,46,47,48Ti, 42,44Ca deduced production σ, systematics. Enriched targets.

doi: 10.1103/PhysRevC.18.2656
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1978KO01      Phys.Rev. C17, 83 (1978)

D.G.Kovar, W.Henning, B.Zeidman, Y.Eisen, J.R.Erskine, H.T.Fortune, T.R.Ophel, P.Sperr, S.E.Vigdor

16O + 48Ca Reaction at 56 Mev. I. Transitions to Resolved Levels

NUCLEAR REACTIONS 48Ca(16O, 16O), (16O, 16O'), (16O, 17O), (16O, 18O), (16O, 14N), 48Ca(16O, 15N), (16O, 16N), (16O, 13C), (16O, 14C), (16O, 15C), (16O, 19O), 48Ca(16O, 17N), (16O, 12C), (16O, 11B), (16O, 12B), (16O, 13B), E=56 MeV; measured σ(θ); deduced optical model parameters. 51,50Ti, 18O, 50Sc, 51V, 48Sc, 49Ti levels deduced reaction population.

doi: 10.1103/PhysRevC.17.83
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1978PA04      Phys.Rev.Lett. 40, 1310 (1978)

M.Paul, S.J.Sanders, J.Cseh, D.F.Geesaman, W.Henning, D.G.Kovar, C.Olmer, J.P.Schiffer

Resonant Effects in the Reaction 24Mg(16O, 12C)28Si

NUCLEAR REACTIONS 24Mg(16O, 12C), E=47, 52, 57 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.40.1310
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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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1978RE02      Phys.Rev.Lett. 40, 1479 (1978)

K.E.Rehm, W.Henning, J.R.Erskine, D.G.Kovar

16O + 40Ca Inelastic Scattering and Direct-Reaction Calculations in Heavy-Ion Scattering

NUCLEAR REACTIONS 40Ca(16O, 16O'), E=60 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.40.1479
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1978TA05      Phys.Rev. C17, 2136 (1978)

S.L.Tabor, D.F.Geesaman, W.Henning, D.G.Kovar, K.E.Rehm, F.W.Prosser, Jr.

Complete Fusion of 16,18O with 24,26Mg

NUCLEAR REACTIONS 24,26Mg(16O, 16O), E=30-81 MeV; 24Mg(18O, 18O), E=32-72 MeV; measured σ(θ); deduced optical model parameters. 24,26Mg(16O, X), E=30-81 MeV; 24Mg(18O, X), E=32-72 MeV; measured total fusion σ(E).

doi: 10.1103/PhysRevC.17.2136
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1977HE02      Phys.Rev. C15, 292 (1977)

W.Henning, Y.Eisen, J.R.Erskine, D.G.Kovar, B.Zeidman

Optical-Model Potential in Single-Nucleon-Transfer Reactions Induced by Heavy Ions

NUCLEAR REACTIONS 48Ca(16O, 16O), (16O, 15N), (19F, 18O), E=56 MeV; 45Sc(15N, 15N), E=47.53 MeV; 48Ca(15N, 14C), E=48 MeV; measured σ(θ). Optical model, DWBA analyses.

doi: 10.1103/PhysRevC.15.292
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1977MA03      Phys.Rev. C15, 161 (1977)

C.F.Maguire, W.D.Callender, D.G.Kovar, C.K.Bockelman

States in 205Pb Excited via the 204Pb(d, p) Reaction. I. The 'Hole' States

NUCLEAR REACTIONS 204Pb(d, p), E=13.0, 20.0 MeV; measured σ(Ep, θ). 205Pb levels deduced S.

doi: 10.1103/PhysRevC.15.161
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1977MA04      Phys.Rev. C15, 170 (1977)

C.F.Maguire, D.G.Kovar, W.D.Callender, C.K.Bockelman

States in 205Pb Excited via the 204Pb(d, p) Reaction. II. The 'Particle' States

NUCLEAR REACTIONS 204Pb(d, p), E=13.0, 20.0 MeV; 208Pb(d, p), E=13.0 MeV; measured σ(Ep, θ). 205Pb deduced levels, S. 208Pb(d, p), E=18.7, 20, 24.8 MeV; 206Pb(d, p), E=17.0 MeV; analyzed previous data. Weak coupling theory.

doi: 10.1103/PhysRevC.15.170
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1977TA07      Phys.Rev. C16, 673 (1977)

S.L.Tabor, Y.Eisen, D.G.Kovar, Z.Vager

Comparison of Light- and Heavy-Ion Emission from the 12C + 16O System

NUCLEAR REACTIONS 12C(16O, p), (16O, α), E=30-64 MeV; measured σ(E, θ). 12C(16O, X), E=35, 49, 62 MeV; measured σ(Z, θ).

doi: 10.1103/PhysRevC.16.673
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1976CH12      Nucl.Phys. A264, 379 (1976)

N.Chirapatpimol, J.C.Fong, M.M.Gazzaly, G.Igo, A.D.Liberman, R.J.Ridge, S.L.Verbeck, C.A.Whitten, Jr., D.G.Kovar, V.Perez-Mendez, N.S.Chant, P.G.Roos

The Quasi-Elastic Knockout of Alpha Particles from 16O and 28Si by 0.65 and 0.85 GeV Alpha Particles

NUCLEAR REACTIONS 16O(α, 2α), E=650, 850 MeV; 28Si(α, 2α), E=850 MeV; measured absolute σ(Eα1, Eα2, θα1, θα2); deduced spectroscopic quantity, N(eff). Results compared with quasi-elastic scattering theories, PWIA, DWIA.

doi: 10.1016/0375-9474(76)90412-7
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1976EI02      Phys.Rev. C13, 699 (1976)

Y.Eisen, H.T.Fortune, W.Henning, D.G.Kovar, S.Vigdor, B.Zeidman

Two-Nucleon Transfer Reactions Induced by 16O on 42Ca and 48Ca

NUCLEAR REACTIONS 42,48Ca(16O, 18O), (16O, 14C), E=56 MeV; measured σ(θ). 44,50Ti, 40,46Ca levels deduced L. 18O, 46Ca, 44,50Ti levels deduced S.

doi: 10.1103/PhysRevC.13.699
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1976SE04      Phys.Rev. C13, 1566 (1976)

R.E.Segel, L.R.Greenwood, P.Debevec, H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, J.E.Monahan, F.J.D.Serduke, T.P.Wangler, W.R.Wharton, B.Zeidman

Prompt Gamma Rays from Nuclear Reactions Induced by 380-MeV π-

NUCLEAR REACTIONS S, Ar, Ca, V, 60Ni, As(π-, X), E=380 MeV; measured σ.

doi: 10.1103/PhysRevC.13.1566
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1976SP03      Phys.Rev.Lett. 36, 405 (1976)

P.Sperr, S.Vigdor, Y.Eisen, W.Henning, D.G.Kovar, T.R.Ophel, B.Zeidman

Oscillations in the Excitation Function for Complete Fusion of 16O + 12C

NUCLEAR REACTIONS 12C(16O, X), E(cm)=13-27 MeV; measured total fusion σ(E).

doi: 10.1103/PhysRevLett.36.405
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1976SP07      Phys.Rev.Lett. 37, 321 (1976)

P.Sperr, T.H.Braid, Y.Eisen, D.G.Kovar, F.W.Prosser, Jr., J.P.Schiffer, S.L.Tabor, S.Vigdor

Fusion Cross Sections of Light Heavy-Ion Systems: Resonances and shell effects

NUCLEAR REACTIONS 12C(12C, X), (18O, X), (19F, X), E(cm)=6-32 MeV; measured fusion σ.

doi: 10.1103/PhysRevLett.37.321
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1975ER02      Phys.Rev.Lett. 34, 680 (1975)

J.R.Erskine, W.Henning, D.G.Kovar, L.R.Greenwood, R.M.DeVries

Nonpeculiar Behavior of the (16O, 12C) Transfer Reaction in the s-d Shell

NUCLEAR REACTIONS 24Mg(16O, 12C), (16O, 16O), E=56 MeV; measured σ(E(12C), θ); deduced potential parameters.

doi: 10.1103/PhysRevLett.34.680
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1975HE01      Phys.Lett. 55B, 49 (1975)

W.Henning, D.G.Kovar, J.R.Erskine, L.R.Greenwood

Spin Determination from Angular Structure of p1/2 Proton Transfer in the 48Ca(15N, 14C)49Sc Reaction

NUCLEAR REACTIONS 48Ca(15N, 14C), E=48 MeV; measured σ(E(14C), θ). 49Sc deduced levels, L, S, J, π.

doi: 10.1016/0370-2693(75)90184-7
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1975HE16      Phys.Lett. 58B, 129 (1975)

W.Henning, J.P.Schiffer, D.G.Kovar, S.Vigdor, B.Zeidman, Y.Eisen, H.-J.Korner

Study of Direct-Reaction Cross Sections in Collisions between Heavy Ions

NUCLEAR REACTIONS 118Sn(18O, 17O), (18O, 16O), (18O, 15N), (18O, 14C), (18O, 13C), (18O, 12C), E=50-62 MeV; 48Ca(16O, X), E=56 MeV; measured σ.

doi: 10.1016/0370-2693(75)90618-8
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1975JA13      Phys.Rev.Lett. 35, 641 (1975)

H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, R.E.Segel, J.P.Schiffer, S.Vigdor, T.P.Wangler, R.L.Burman, D.M.Drake, P.A.M.Gram, R.P.Redwine, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark

Systematics of Pion and Proton Interactions with Ni Nuclides

NUCLEAR REACTIONS 58,60Ni(π+, X), (π-, X), E=220 MeV; 58,60Ni(p, X), E=200 MeV; 58Ni(π+, X), E=100 MeV; measured σ(fragment) from γ-spectra.

doi: 10.1103/PhysRevLett.35.641
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1975JA15      Phys.Rev.Lett. 35, 1170 (1975)

H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, S.E.Vigdor, T.P.Wangler, R.E.Segel, J.P.Schiffer, R.L.Burman, P.A.M.Gram, D.M.Drake, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark

Absolute Cross Sections for Production of Prompt Nuclear γ Rays by Fast Pions

NUCLEAR REACTIONS 27Al(π+, X), E=100 MeV; 51V, 40Ca(π-, X), E=220 MeV; 60Ni(π-, X), (π+, X), E=380 MeV; measured σ(Eγ).

doi: 10.1103/PhysRevLett.35.1170
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1974BE16      Phys.Rev. C9, 1543 (1974)

F.D.Becchetti, D.G.Kovar, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, W.von Oertzen, N.K.Glendenning

Two-Proton-Transfer Reactions 208Pb(12C, 10Be)210Po and 208Pb(16O, 14C)210Po

NUCLEAR REACTIONS 208Pb(12C, 10Be), (16O, 14C), E(12C)=78 MeV, E(16O)=104, 140 MeV; 209Bi(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104 MeV; measured σ(Eout, θ). 210Po levels deduced relative strengths.

doi: 10.1103/PhysRevC.9.1543
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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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1974HE05      Phys.Rev.Lett. 32, 1015 (1974)

W.Henning, D.G.Kovar, B.Zeidman, J.R.Erskine

L Dependence in Angular Distributions of the Two-Proton Transfer Reaction 48Ca(16O, 14C)50Ti

NUCLEAR REACTIONS 48Ca(16O, 14C), E=56 MeV; measured σ(E(14C), θ). 50Ti levels deduced L.

doi: 10.1103/PhysRevLett.32.1015
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1974KO20      Nucl.Phys. A231, 266 (1974)

D.G.Kovar, N.Stein, C.K.Bockelman

Excitation of Two-Particle-One-Hole States by the 208Pb(d, p)209Pb Reaction

NUCLEAR REACTIONS 208Pb(d, p), E=20 MeV; measured σ(Ep, θ); deduced Q. 209Pb deduced levels, J, π, S, L. Enriched targets.

doi: 10.1016/0375-9474(74)90522-3
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1974KO25      Phys.Rev.Lett. 33, 1611 (1974)

D.G.Kovar, W.Henning, B.Zeidman, Y.Eisen, H.T.Fortune

Measurement of the Reaction 48Ca(16O, 15C)49Ti

NUCLEAR REACTIONS 48Ca(16O, 15C), E=56 MeV; measured σ(E(15C), θ); deduced Q.

doi: 10.1103/PhysRevLett.33.1611
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1974MA19      Phys.Rev.Lett. 32, 1452 (1974)

B.Mayer, H.E.Conzett, W.Dahme, D.G.Kovar, R.M.Larimer, C.Leemann

j Dependence of the Vector Analyzing Power for (d, 3He) and (d, t) Reactions

NUCLEAR REACTIONS 208Pb(d, 3He), (d, t), E=30 MeV; measured σ(E(3He), Et, θ), Ay(E(3He), Et, θ). 207Pb deduced J, π, J dependence of vector analyzing power.

doi: 10.1103/PhysRevLett.32.1452
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1973HE05      Phys.Rev.Lett. 30, 571 (1973)

D.L.Hendrie, B.G.Harvey, J.R.Meriwether, J.Mahoney, J.-C.Faivre, D.G.Kovar

Multipole Deformation of 238U

NUCLEAR REACTIONS 238U(α, α), (α, α'), E=50 MeV; measured σ(θ). 238U deduced deformation parameters β(L).

doi: 10.1103/PhysRevLett.30.571
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1973KO09      Phys.Rev.Lett. 30, 1075 (1973)

D.G.Kovar, B.G.Harvey, F.D.Becchetti, J.Mahoney, D.L.Hendrie, H.Homeyer, W.von Oertzen, M.A.Nagarajan

Evidence for Recoil Effects in Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS 208Pb(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104, 140 MeV; measured σ(E(11B), E(15N), θ); deduced recoil effects. 209Bi levels deduced S.

doi: 10.1103/PhysRevLett.30.1075
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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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1972BE75      Phys.Rev. C6, 2215 (1972)

F.D.Becchetti, D.G.Kovar, B.G.Harvey, J.Mahoney, B.Mayer, F.G.Puhlhofer

Inelastic Scattering of 16O from 208Pb

NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=104 MeV; measured σ(θ). 208Pb deduced levels, β, B(EL).

doi: 10.1103/PhysRevC.6.2215
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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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