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Search: Author = J.B.Ball

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1994BA23      Nucl.Phys. A570, 15c (1994)

J.B.Ball

The Future Radioactive Ion Beam Research Program at Oak Ridge

doi: 10.1016/0375-9474(94)90265-8
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1990KO27      Nucl.Phys. A516, 133 (1990)

M.Korolija, N.Cindro, R.Caplar, R.L.Auble, J.B.Ball, R.L.Robinson

Master-Equation Analysis of Proton Spectra from 16O- and 58Ni-Induced Reactions

NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(16O, pX), E=25.2 MeV/nucleon; 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(58Ni, pX), E=15.1 MeV/nucleon; measured angle integrated proton spectra. Master equation analysis.

doi: 10.1016/0375-9474(90)90053-O
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1988AU01      Phys.Rev. C37, 390 (1988)

R.L.Auble, J.B.Ball, F.E.Bertrand, R.L.Ferguson, I.Y.Lee, R.L.Robinson, G.R.Young

Target/Projectile Mass Dependence of Light Ion Yields from Heavy Ion Collisions

NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120Sn, 197Au(16O, X), E=403 MeV; 27Al, 46Ti, 60Ni, 120Sn, 197Au(32S, X), E=504, 680 MeV; 27Al, 46Ti, 60Ni, 120Sn, 197Au(58Ni, X), E=876 MeV; measured σ(E, θ) for X=p, d, t, α; deduced integral yields.

doi: 10.1103/PhysRevC.37.390
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1988DA11      J.Phys.(London) G14, 937 (1988)

S.Datta, R.Caplar, N.Cindro, R.L.Auble, J.B.Ball, R.L.Robinson

A Refined Coalescence Model for Intermediate-Energy Heavy-Ion Collisions. Application to Deuteron Spectra

NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(16O, dX), (32S, dX), (58Ni, dX), E=15-25 MeV/nucleon; measured σ(Ed, θ). Coalescence-model analysis.

doi: 10.1088/0305-4616/14/7/012
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1988KO26      Nucl.Phys. A487, 442 (1988)

M.Korolija, N.Cindro, R.Caplar, R.L.Auble, J.B.Ball, R.L.Robinson

Determination of the Initial Number of Degrees of Freedom in Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(32S, pX), E=503.7, 678.8 MeV; analyzed σ(Ep, θp) data; deduced reaction mechanism.

doi: 10.1016/0375-9474(88)90623-9
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1987DA15      Phys.Lett. 192B, 302 (1987)

S.Datta, R.Caplar, N.Cindro, R.L.Auble, J.B.Ball, R.L.Robinson

Coalescence-Model Analysis of Alpha-Particle and Deutron Spectra from Energetic Heavy-Ion Collisions

NUCLEAR REACTIONS 27Al, 46Ti, 60Ni, 120,124Sn, 197Au(16O, α), (32S, α), (58Ni, α), 46Ti, 197Au(16O, d), 197Au(32S, d), 60Ni(58Ni, d), E=15-25 MeV/nucleon; calculated σ(Eα, θα), σ(Ed, θd); deduced coalescence radii. Coalescence model.

doi: 10.1016/0370-2693(87)90110-9
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1987KO25      Z.Phys. A327, 237 (1987)

M.Korolija, N.Cindro, R.Caplar, R.L.Auble, J.B.Ball, R.L.Robinson

Multiple-Source Analysis of Inclusive Proton Spectra from 58Ni + 60Ni Collisions at 876.5 MeV

NUCLEAR REACTIONS 60Ni(58Ni, pX), E=876.5 MeV; measured inclusive σ(Ep, θp). Multiple moving source analysis.


1983AU06      Phys.Rev. C28, 1552 (1983)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, C.Y.Wong, D.L.Hendrie, H.D.Holmgren, J.D.Silk

Light Ion Emission from Reactions Induced by 0.8-2.4 GeV 16O Projectiles

NUCLEAR REACTIONS Ni(16O, X), E=0.8, 1.6, 2.4 GeV; Au(16O, X), E=1.6, 2.4 GeV; Al, Sn(16O, X), E=1.6 GeV; measured σ(E, θ) for X=p, d, t, 3He, 4He; deduced model parameters.

doi: 10.1103/PhysRevC.28.1552
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1983RO10      Phys.Rev. C27, 3006 (1983)

R.L.Robinson, R.L.Auble, J.B.Ball, F.E.Bertrand, R.L.Ferguson, C.B.Fulmer, J.Gomez del Campo, I.Y.Lee, R.W.Novotny, G.R.Young, J.C.Wells, C.F.Maguire, H.Yamada

Nucleon Multiplicity Associated with Energetic Protons from the 12C + 60Ni Reaction

NUCLEAR REACTIONS 60Ni(12C, pX), E=191 MeV; measured (fragment)p-coin, charged particle multiplicities; deduced reaction mechanism.

doi: 10.1103/PhysRevC.27.3006
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1983SA20      Phys.Lett. 128B, 147 (1983)

G.R.Satchler, C.B.Fulmer, R.L.Auble, J.B.Ball, F.E.Bertrand, K.A.Erb, E.E.Gross, D.C.Hensley

Refractive Effects in 9Be Scattering and Nuclear Rainbow Ghosts

NUCLEAR REACTIONS 12C, 16O(9Be, 9Be), E=158 MeV; measured σ(θ); deduced optical model parameters, nuclear rainbow, refractive effects. Optical model.

doi: 10.1016/0370-2693(83)90378-7
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1982AU04      Phys.Rev. C25, 2504 (1982)

R.L.Auble, J.B.Ball, F.E.Bertrand, R.L.Ferguson, C.B.Fulmer, I.Y.Lee, R.L.Robinson, G.R.Young, J.R.Wu, J.C.Wells, H.Yamada

Light-Ion Emission in Heavy-Ion Collision: Beam energy dependence

NUCLEAR REACTIONS 60Ni(12C, pX), (12C, dX), (12C, tX), (12C, 3HeX), (12C, αX), E=90, 123, 156, 189 MeV; measured σ(θp), σ(θd), σ(θα), σ(θ(3He)) vs E; deduced integral yields, model parameters. Moving source model.

doi: 10.1103/PhysRevC.25.2504
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1982AU07      Phys.Rev.Lett. 49, 441 (1982)

R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, D.L.Hendrie, H.D.Holmgren, J.D.Silk, H.Breuer

Target-A Dependence of Light-Ion Emission from Reactions Induced by 100-MeV/u 16O

NUCLEAR REACTIONS Al, Ni, Sn, Au(16O, p), (16O, d), (16O, t), (16O, 3He), (16O, α), E=100 MeV/nucleon; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα), inclusive reactions; deduced reaction mechanism, moving source parameters, target mass effects.

doi: 10.1103/PhysRevLett.49.441
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1982FU09      Nucl.Phys. A385, 83 (1982)

C.B.Fulmer, S.Mukhopadhyay, G.R.Satchler, R.L.Auble, J.B.Ball, F.E.Bertrand, E.E.Gross, D.C.Hensley

Elastic and Inelastic Scattering of 79.5 MeV 11B and 87.5 MeV 10B Ions

NUCLEAR REACTIONS 24,25,26Mg, 27Al, 59Co, 60Ni, 197Au(11B, 11B), 24,26Mg(11B, 11B'), E=79.5 MeV; 24,25Mg, 60Ni(10B, 10B), 24Mg, 60Ni(10B, 10B'), E=87.5 MeV; measured σ(θ); deduced optical model parameters. 26Mg(11B, 11B), (11B, 10B), (11B, 12B), (11B, 13C), (11B, 12C), (11B, 11C), (11B, 9Be), (11B, 10Be), (11B, 7Be), (11B, 7Li), (11B, 6Li), (11B, 8Li), E=79.6 MeV; measured σ(θ) vs reaction product E.

doi: 10.1016/0375-9474(82)90491-2
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1981FU05      Phys.Lett. 100B, 305 (1981)

C.B.Fulmer, J.B.Ball, R.L.Ferguson, R.L.Robinson, J.R.Wu

Light Particle Emission from Reactions of 208 MeV 16O Ions with 12C, 56Fe, and 91Zr

NUCLEAR REACTIONS 12C, 56Fe, 91Zr(16O, p), (16O, d), (16O, t), (16O, 3He), (16O, α), E=208.2 MeV; measured σ(θ, Ep), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα); deduced projectile breakup contributions. Modified fireball model.

doi: 10.1016/0370-2693(81)90092-7
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1981RO11      Phys.Rev. C24, 2084 (1981)

R.L.Robinson, R.L.Auble, I.Y.Lee, M.J.Martin, G.R.Young, J.Gomez del Campo, J.B.Ball, F.E.Bertrand, R.L.Ferguson, C.B.Fulmer, J.R.Wu, J.C.Wells, H.Yamada

Fast Proton and Alpha Particles from the 12C + 60Ni Reaction

NUCLEAR REACTIONS 60Ni(12C, pX), (12C, αX), E=136, 194 MeV; measured Eγ, Iγ, αγ-, α(fragment)-, p(fragment)-coin, (particle)(particle)(θ), γ-multiplicities; deduced light-ion production mechanism.

doi: 10.1103/PhysRevC.24.2084
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1980RE04      Nucl.Phys. A346, 371 (1980)

A.C.Rester, J.B.Ball, R.L.Auble

Nuclear Structure Study of States in 72Ge and 74Ge with (p, t) Reactions

NUCLEAR REACTIONS 74,76Ge(p, t), E=35.4 MeV; measured σ(θ). 72,74Ge deduced levels, L, J, π. Enriched targets. DWBA analyses.

doi: 10.1016/0375-9474(80)90475-3
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1978BA22      Phys.Rev.Lett. 40, 1698 (1978)

J.B.Ball, C.B.Fulmer, M.L.Mallory, R.L.Robinson

Protons, Deuterons, and Tritons Emitted from the Reaction of 192-MeV 12C with 56Fe

NUCLEAR REACTIONS 56Fe(12C, X), E=192 MeV; measured σ(Z, θ), Z=1, 7.

doi: 10.1103/PhysRevLett.40.1698
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1976RA26      Phys.Rev. C14, 1381 (1976)

S.Raman, R.L.Auble, J.B.Ball, E.Newman, J.C.Wells, Jr., J.Lin

Levels in 144Nd from the 143Nd(d, p) and 146Nd(p, t) Reactions

NUCLEAR REACTIONS 143Nd(d, p), E=25 MeV; measured σ(θ). 146Nd(p, t), E=31 MeV; measured σ(θ). 144Nd deduced levels, L, S. DWBA analysis.

doi: 10.1103/PhysRevC.14.1381
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1975BA22      Nucl.Phys. A244, 341 (1975)

J.B.Ball, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

16O Induced One-Nucleon Transfer Reactions on Targets of 26Mg, 27Al, 30Si and 48Ca

NUCLEAR REACTIONS 26Mg, 27Al, 30Si, 48Ca(16O, 16O), E=60 MeV; 24Mg, 27Al, 30Si(16O, 16O), E=45 MeV; measured σ(θ). 48Ca(16O, 15N), E=56 MeV; 30Si(16O, 15N), E=50 MeV; 26Mg, 27Al, 30Si(16O, 15N), E=45, 60 MeV; measured σ(E(15N), θ). 48Ca(16O, 17O), E=60 MeV; measured σ(E(17O), θ). 27Al(16O, 17F), E=60 MeV; measured σ(E(17F), θ). 26Mg, 27Al, 28Si, 31P, 47Ca, 49Sc levels deduced L. DWBA analysis.

doi: 10.1016/0375-9474(75)90064-0
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1975BA62      Nucl.Phys. A252, 208 (1975)

J.B.Ball, C.B.Fulmer, E.E.Gross, M.L.Halbert, D.C.Hensley, C.A.Ludemann, M.J.Saltmarsh, G.R.Satchler

Heavy Ion Elastic Scattering Survey (I). 208Pb Target

NUCLEAR REACTIONS 208Pb(12C, 12C), E=96 MeV; 208Pb(16O, 16O), E=129.5, 192 MeV; 208Pb(20Ne, 20Ne), E=161.2 MeV; measured σ(θ); deduced optical parameters. 208Pb(12C, 12C), E=116.4 MeV; 208Pb(11B, 11B), E=72.2 MeV; 207,208Pb, 209Bi(α, α), E=42 MeV; analyzed σ(θ); deduced optical parameters.

doi: 10.1016/0375-9474(75)90613-2
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1975HI03      Phys.Rev. C12, 260 (1975)

D.L.Hillis, C.R.Bingham, D.A.McClure, N.S.Kendrick, Jr., J.C.Hill, S.Raman, J.B.Ball, J.A.Harvey

Nuclear Spectroscopy of 145Nd

RADIOACTIVITY 145Pr; measured Eγ, Iγ, γγ-coin; deduced log ft. 145Nd deduced levels, J, π.

NUCLEAR REACTIONS 144Nd(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin. 144Nd(d, p), E=33.3 MeV; measured σ(Ep, θ). 144Nd(α, 3He), E=66.2 MeV; measured σ(E(3He)). 146Nd(p, d), E=31 MeV; measured σ(Ed, θ). 145Nd deduced levels, J, π, L, S, neutron separation, γ-branching.

doi: 10.1103/PhysRevC.12.260
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1974BA31      Phys.Lett. 49B, 348 (1974)

J.B.Ball, O.Hansen, J.S.Larsen, D.Sinclair, F.Videbaek

The (16O, 15N) Reaction at Forward Angles

NUCLEAR REACTIONS 26Mg, 30Si(16O, 15N), E=45 MeV; 48Ca(16O, 15N), E=56 MeV; measured σ(E(15N), θ).

doi: 10.1016/0370-2693(74)90178-6
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1974EI03      Phys.Rev. C10, 1572 (1974)

E.Eichler, G.D.O'Kelley, J.S.Eldridge, J.B.Ball

Search for the Decay of 96Zr

RADIOACTIVITY 96Zr; measured lower limit for T1/2.

doi: 10.1103/PhysRevC.10.1572
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1974VO11      Phys.Lett. 52B, 187 (1974)

G.Vourvopoulos, M.B.Greenfield, J.B.Ball, S.Raman, W.K.Dagenhart

Two-Step Mechanism in the 22Ne(p, t) Reaction

NUCLEAR REACTIONS 22Ne(p, t), E=40 MeV; measured σ(Et, θ); deduced reaction mechanism to 2- level of 20Ne.

doi: 10.1016/0370-2693(74)90085-9
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1973BA26      Nucl.Phys. A207, 425 (1973)

J.B.Ball, C.B.Fulmer, J.S.Larsen, G.Sletten

Energy Levels of 94Ru Observed with the 96Ru(p, t) Reaction

NUCLEAR REACTIONS 96Ru(p, t), E=31.1 MeV; measured σ(Et, θ). 94Ru deduced levels, L(2n), J, π. Enriched target.

doi: 10.1016/0375-9474(73)90356-4
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1973BA56      Phys.Rev. C8, 1438 (1973)

J.B.Ball, J.J.Pinajian, J.S.Larsen, A.C.Rester

Study of 82Sr, 84Sr, and 86Sr with the (p, t) Reaction

NUCLEAR REACTIONS 84,86,87,88Sr(p, t), E=31 MeV; measured σ(Et, θ). Deduced Q. 82,84,86Sr deduced levels, J, π, L, enhancement factors.

doi: 10.1103/PhysRevC.8.1438
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1973HE02      Nucl.Phys. A201, 225 (1973)

V.D.Helton, J.C.Hiebert, J.B.Ball

Neutron Hole States in 138La and 140Pr

NUCLEAR REACTIONS 139La(p, d), E=31.6 MeV; 141Pr(p, d), E=30.0 MeV; 142Nd(p, d), 144Sm(p, d), E=29.5 MeV; measured σ(Ed, θ), 138La, 140Pr deduced levels, L(n), J, π, spectroscopic strengths. 139La(p, p), 141Pr(p, p), E=29.3-30.0 MeV; 141Pr(d, d), E=22.7 MeV; measured σ(E, θ). Optical-model analysis; deduced potentials. Natural, enriched targets.

doi: 10.1016/0375-9474(73)90063-8
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1973LA04      Phys.Rev. C7, 751 (1973)

J.S.Larsen, J.B.Ball, C.B.Fulmer

Level Structure of 92Mo and 94Mo Studied with the (p, t) Reaction

NUCLEAR REACTIONS 94,96Mo(p, t), E=31 MeV; measured σ(Et, θ). 92,94Mo deduced levels, J, π, L.

doi: 10.1103/PhysRevC.7.751
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1973RA25      Nucl.Phys. A208, 371 (1973)

J.Rapaport, J.B.Ball, R.L.Auble

The 48Ti(p, t)46Ti Reaction

NUCLEAR REACTIONS 48Ti(p, t), E=51 MeV; measured σ(Et, θ). 46Ti deduced levels, L, J, π, enhancement factors.

doi: 10.1016/0375-9474(73)90382-5
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1972AU02      Nucl.Phys. A179, 353 (1972)

R.L.Auble, J.B.Ball

Energy Levels of 122,124Te Populated by (3He, d) and (p, t) Reactions

NUCLEAR REACTIONS 121,123Sb(3He, d), E=25 MeV; 124,126Te(p, t), E=33 MeV; measured σ(Ed, θ), σ(Et, θ). 122,124Te deduced levels, J, π, L(p), L(2n), S.

doi: 10.1016/0375-9474(72)90375-2
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1972AU05      Phys.Rev. C6, 2223 (1972)

R.L.Auble, D.J.Horen, F.E.Bertrand, J.B.Ball

Proton Excitations in 108,110Cd from (3He, d) Reactions

NUCLEAR REACTIONS 107,109Ag(3He, d), E=27 MeV; measured σ(Ed, θ). 108,110Cd deduced levels, J, π, S.

doi: 10.1103/PhysRevC.6.2223
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1972BA49      Phys.Lett. 41B, 55 (1972)

J.B.Ball

A Remark on the Level Structure of 93Mo and the Failure of j-Determination by Spectroscopic Factor Ratios Near Closed Shells

NUCLEAR REACTIONS 95Mo(p, t), E=3.1 MeV; measured σ(θ). 93Mo deduced levels, L, J, π, S.

doi: 10.1016/0370-2693(72)90367-X
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1972BA75      Phys.Rev.Lett. 29, 1014 (1972)

J.B.Ball, J.S.Larsen

Systematics of L = 0 Transitions Observed in the (p, t) Reaction of Nuclei Near N = 50

NUCLEAR REACTIONS 88Sr, 96Ru, 90,92Zr, 92,94Mo(p, t), E=31 MeV; measured σ(Et). 86Sr, 94Ru, 88,90Zr, 90,92Mo deduced L=0 strength systematics.

doi: 10.1103/PhysRevLett.29.1014
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1972BB03      Phys.Rev. C6, 2139 (1972)

J.B.Ball

91Zr(p, t) Reaction and the Level Structure of 89Zr

NUCLEAR REACTIONS 91Zr(p, t), E=31 MeV; measured σ(θ). 89Zr deduced levels, J, π, L.

doi: 10.1103/PhysRevC.6.2139
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1972BB08      Phys.Lett. 41B, 581 (1972)

J.B.Ball, J.B.McGrory, J.S.Larsen

Calculated Energy Levels for 89Y, 90Zr, 91Nb, 92Mo, 93Tc and 94Ru

NUCLEAR STRUCTURE 89Y, 90Zr, 91Nb, 92Mo, 93Tc, 94Ru; calculated levels, binding energies. Shell model, inert 88Sr core.

doi: 10.1016/0370-2693(72)90639-9
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1972LA38      Phys.Lett. 42B, 205 (1972)

J.S.Larsen, J.L.C.Ford, Jr., R.M.Gaedke, K.S.Toth, J.B.Ball, R.L.Hahn

Investigation of the 208Pb(12C, 11B)209Bi and 208Pb(12C, 13C)207Pb Reactions at High Bombarding Energies

NUCLEAR REACTIONS 208Pb(12C, 11B), (12C, 13C), E=77, 98, 116 MeV; measured σ(θ); analyzed reaction mechanisms.

doi: 10.1016/0370-2693(72)90061-5
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1972MC02      Phys.Rev. C5, 145 (1972)

C.M.McKenna, K.W.Kemper, J.D.Fox, J.W.Nelson, J.B.Ball

Levels of 50Mn from the Reaction 50Cr(3He, t)50Mn

NUCLEAR REACTIONS 50Cr(3He, t), E=39.45 MeV; measured σ(Et, θ). 50Mn deduced levels, J, π.

doi: 10.1103/PhysRevC.5.145
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1972RA05      Phys.Rev. C5, 453 (1972)

J.Rapaport, J.B.Ball, R.L.Auble, T.A.Belote, W.E.Dorenbusch

Level Structure of 44Ti

NUCLEAR REACTIONS 46Ti(p, t), E=51 MeV; measured σ(Et, θ), Q. 44Ti deduced levels, J, π, L, isobaric analog.

doi: 10.1103/PhysRevC.5.453
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1972RA14      Nucl.Phys. A184, 138 (1972)

S.Raman, R.L.Auble, W.T.Milner, J.B.Ball, F.K.McGowan, P.H.Stelson, R.L.Robinson

Nuclear Spectroscopy of 50Cr

RADIOACTIVITY 50Mn; measured T1/2, Eγ, Iγ.

NUCLEAR REACTIONS 50Cr(p, p'γ), E=8.4 MeV; measured Eγ, Iγ. 52Cr(p, t), E=31.4 MeV; measured σ(Et, θ). 50Cr(35Cl, 35Cl'γ), E=54 MeV; measured B(E2), Doppler shift attenuation. 50Cr deduced levels, J, π, γ-branching, T1/2.

doi: 10.1016/0375-9474(72)90449-6
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1971BA01      Nucl.Phys. A160, 225 (1971)

J.B.Ball

Studies of 95Ru and 94Ru with the 96Ru(p, d) and (p, t) Reactions

NUCLEAR REACTIONS 96Ru(p, d), 96Ru(p, t), Ep=31.5 MeV; measured Q, σ(E, θ). 95Ru deduced levels, L(n), J, π, spectroscopic strengths, ground state mass excess. 94Ru deduced ground state mass excess. Enriched target.

doi: 10.1016/0375-9474(71)90127-8
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1971BA43      Phys.Rev. C4, 196 (1971)

J.B.Ball, R.L.Auble, P.G.Roos

Study of the Zirconium Isotopes with the (p, t) Reaction

NUCLEAR REACTIONS 90,91,92,94,96Zr(p, t), E=38 MeV; measured σ(Et, θ), Q. 88,89,90,92,94Zr deduced levels, J, π, L.

doi: 10.1103/PhysRevC.4.196
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1971DO18      Phys.Lett. 37B, 173 (1971)

W.E.Dorenbusch, J.B.Ball, R.L.Auble, J.Rapaport, T.A.Belote

Energy Levels in 48Cr Observed in the 50Cr(p, t)48Cr Reaction

NUCLEAR REACTIONS 50Cr(p, t), E=51 MeV; measured σ(Et, θ), Q. 48Cr deduced levels, isobaric analogs, L, J, π.

doi: 10.1016/0370-2693(71)90043-8
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1971DU02      Phys.Rev. C3, 1391 (1971)

J.L.DuBard, R.K.Sheline, J.B.Ball

Three-Quasiparticle States in 139La

NUCLEAR REACTIONS 138La(d, p), E=12 MeV; measured Q, σ(Ep, θ). 139La deduced levels, L(n).

doi: 10.1103/PhysRevC.3.1391
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1969BA08      Phys.Rev. 177, 1699 (1969)

J.B.Ball, R.L.Auble, R.M.Drisko, P.G.Roos

Level Structure of 88Zr Studied with the 90Zr(p, t) Reaction

NUCLEAR REACTIONS 90Zr(p, t), E=31 MeV; measured σ(Et, θ). 88Zr deduced levels, J, π, L, S. Enriched target.

doi: 10.1103/PhysRev.177.1699
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1969BA13      Phys.Letters 29B, 172 (1969)

J.B.Ball, R.L.Auble, P.G.Roos

The (p, t) Reaction on the Even Zirconium Isotopes

NUCLEAR REACTIONS 90Zr, 92Zr, 94Zr, 96Zr(p, t), E=38 MeV; measured σ(Et, θ). 88Zr, 90Zr, 92Zr, 94Zr deduced levels, L.

doi: 10.1016/0370-2693(69)90011-2
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1969BA45      Phys.Letters 30B, 533 (1969)

J.B.Ball, R.L.Auble, J.Rapaport, C.B.Fulmer

Levels in 140,142,144Nd and a Search for Pairing Vibrations at N = 82 with the (p, t) Reaction

NUCLEAR REACTIONS 142,144,146Nd(p, t), E = 31 MeV; measured σ(Et, θ). 140,142,144Nd deduced L=0 transition strengths.

doi: 10.1016/0370-2693(69)90448-1
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1969CA20      Phys.Rev. 187, 1682 (1969)

M.R.Cates, J.B.Ball, E.Newman

Nuclear-Structure Studies of 91,92,93,95,97Nb and 94Mo with the (3He, d) Reaction

NUCLEAR REACTIONS 93Nb, 90,91,92Zr(3He, d), E=30.9 MeV; 90,94,96Zr(3He, d), E=24.7 MeV; measured σ(Ed, θ). 94Mo, 91,92,93,95,97Nb deduced levels, J, π, L(p), S.

doi: 10.1103/PhysRev.187.1682
Citations: PlumX Metrics


1969FU07      Phys.Rev. 181, 1565 (1969)

C.B.Fulmer, J.B.Ball, A.Scott, M.L.Whiten

Elastic Scattering of 61.4-MeV Protons

NUCLEAR REACTIONS 12C, 27Al, 40Ca, 58Ni, 68Zn, 90Zr, 116Sn, 208Pb(p, p), E = 61.4 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1103/PhysRev.181.1565
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0211.


1968AU01      Phys.Rev. 169, 955 (1968)

R.L.Auble, J.B.Ball, C.B.Fulmer

Levels in Odd-Mass Sb and I Isotopes Studied with the (3He, d) Reaction

NUCLEAR STRUCTURE 51Cr, 125Sb, 127I, 131I, 129I; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.169.955
Citations: PlumX Metrics


1968AU04      Nucl.Phys. A116, 14 (1968)

R.L.Auble, J.B.Ball, C.B.Fulmer

The (d, 3He) Reaction on 126Te, 128Te and 130Te Nuclei

NUCLEAR REACTIONS 126,128,130Te(d, 3He), E=34 MeV; measured σ(E(3He), θ). 125,127,129Sb deduced levels, L, π, J. Enriched targets.

doi: 10.1016/0375-9474(68)90478-8
Citations: PlumX Metrics


1968BA31      Phys.Rev. 172, 1199 (1968)

J.B.Ball, C.B.Fulmer

Neutron Hole States in Z = 40 Nuclei Studied with the (p, d) Reaction on 90Zr, 91Zr, and 92Zr

NUCLEAR REACTIONS 90,91,92Zr(p, d), E=31 MeV; measured σ(Ed, θ); deduced Q. 89,90,91Zr deduced levels, J, π.

doi: 10.1103/PhysRev.172.1199
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0322.


1967BA30      Phys.Letters 25B, 126 (1967)

J.B.Ball, M.R.Cates

The 91Zr(3He, d) Reaction to the Positive and Negative Parity Low-Lying States in 92Nb

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90201-8
Citations: PlumX Metrics


1967MA37      Phys.Rev.Letters 19, 1449 (1967)

M.D.Mancusi, C.M.Jones, J.B.Ball

Search for Excited States in 3He

NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.1449
Citations: PlumX Metrics


1967SC24      Phys.Lett. 25B, 463 (1967)

A.Scott, M.L.Whiten, J.B.Ball

Excitation of the 0.908 MeV Level in 89Y by Inelastic Scattering of 61.2 MeV Protons

NUCLEAR STRUCTURE 89Y; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90108-6
Citations: PlumX Metrics


1965BA02      Bull.Am.Phys.Soc. 10, No.1, 121, KD4 (1965)

J.B.Ball, R.F.Sweet

Low-Lying Levels in 50V and 58Co Studied with the (p, d) Reaction

NUCLEAR STRUCTURE 50V, 58Co; measured not abstracted; deduced nuclear properties.


1965BA29      Phys.Rev. 140, B904 (1965)

J.B.Ball, R.F.Sweet

Low-Lying Levels in 50V and 58Co Studied with the (p, d) Reaction

NUCLEAR STRUCTURE 50V, 58Co, 56Co; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B904
Citations: PlumX Metrics


1965BA53      ORNL-3940, p.36 (1965)

J.B.Ball

Nuclear Spectroscopy with (p, α) Reactions

NUCLEAR STRUCTURE 87Y, 86Sr; measured not abstracted; deduced nuclear properties.


1965BH01      Nucl.Phys. 63, 286 (1965)

K.H.Bhatt, J.B.Ball

Nuclear Spectroscopy of the Isotopes of Nb, Mo and Tc

NUCLEAR STRUCTURE 93Nb, 93Tc, 93Mo, 94Tc, 94Nb, 94Mo, 96Nb, 96Mo, 95Tc, 95Nb, 95Mo; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(65)90344-5
Citations: PlumX Metrics


1965FU09      Phys.Rev. 140, B330 (1965)

C.B.Fulmer, J.B.Ball

Direct-Interaction (p, α) Reactions in 89Y and 90Zr

NUCLEAR STRUCTURE 86Sr, 87Y; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.140.B330
Citations: PlumX Metrics


1965GR10      Nucl.Phys. 67, 433 (1965)

U.Gruber, R.Koch, B.P.Maier, O.W.B.Schult, J.B.Ball, K.H.Bhatt, R.K.Sheline

Energies and Character of Low-Lying Levels in Nb94

NUCLEAR REACTIONS 93Nb(n, γ), E=pile; measured Eγ, Iγ. 94Nb deduced levels.

doi: 10.1016/0029-5582(65)90823-0
Citations: PlumX Metrics


1965SH03      Nucl.Phys. 61, 342 (1965)

R.K.Sheline, R.T.Jernigan, J.B.Ball, K.H.Bhatt, Y.E.Kim, J.Vervier

The 93Nb(d, p)94Nb Reaction and the Low-Lying States of 94Nb

NUCLEAR REACTIONS 93Nb(d, p), E=10.2-12.2 MeV; measured σ(E; Ep, θ), Q. 94Nb deduced levels. Natural target.

doi: 10.1016/0029-5582(65)90908-9
Citations: PlumX Metrics


1964BA56      Phys.Rev. 135, B706 (1964)

J.B.Ball, C.B.Fulmer, R.H.Bassel

Scattering of 22.5-MeV Protons from Zirconium and the Symmetry Term in the Nuclear Optical Potential

NUCLEAR REACTIONS 90,91,92,94,96Zr(p, p), E=22.5 MeV; measured products, 90Zr, 91Zr, 92Zr, 94Zr, 96Zr; deduced σ(θ). Data were imported from EXFOR entry C0085.

doi: 10.1103/PhysRev.135.B706
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0085.


1964FU02      Bull.Am.Phys.Soc.9, No.1, 94, JC15 (1964)

C.B.Fulmer, J.B.Ball

(p, α) Reactions on Y89 and Zr90 at 22.5 MeV

NUCLEAR STRUCTURE 86Sr, 87Y; measured not abstracted; deduced nuclear properties.


1964SW01      Phys.Lett. 8, 131 (1964)

R.F.Sweet, K.H.Bhatt, J.B.Ball

The Low-Lying Levels in Nb92 and the Ground State of Nb93

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90739-5
Citations: PlumX Metrics


1964SW03      Bull.Am.Phys.Soc. 9, No.4, 483, JA3 (1964)

R.F.Sweet, J.B.Ball, C.D.Goodman, K.H.Bhatt

Measurement and Nuclear-Shell-Model Interpretation of the Low-Lying States of 92Nb

NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.


1963BA02      Bull.Am.Phys.Soc. 8, No.1, 60, R9 (1963)

J.B.Ball, C.B.Fulmer

Scattering of 22.5-MeV Protons from Separated Isotopes of Zirconium

NUCLEAR STRUCTURE 94Zr, 96Zr, 92Zr, 90Zr, 91Zr; measured not abstracted; deduced nuclear properties.


1963BA33      Phys.Rev. 130, 2341 (1963)

J.B.Ball, C.B.Fulmer, C.D.Goodman

(p, d), (p, t), and (p, α) Reactions to the Same Final States in Fe56 and in Zr90

NUCLEAR STRUCTURE 90Zr, 56Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.130.2341
Citations: PlumX Metrics


1963BA78      Phys.Rev. 130, 2342 (1963)

J.B.Ball, C.B.Fulmer, C.D.Goodman

(p, d), (p, t), and (p, α) Reaction to the Same Final States in Fe56 and in Zr90

NUCLEAR REACTIONS 57Fe(p, d), 58Fe(p, t), 59Co(p, α), E=22.3 MeV; measured products, 56Fe, 2H, 3H, 4He; deduced σ(θ, E), σ(θ). Data were imported from EXFOR entry C1034.

doi: 10.1103/PhysRev.130.2342
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1034.


1962BA01      Bull.Am.Phys.Soc. 7, No.1, 83, Y9 (1962)

J.B.Ball, C.D.Goodman, C.B.Fulmer

A Comparison of Cross-Sections for (p, d), (p, t) and (p, α) to the Same Final States

NUCLEAR STRUCTURE 90Zr, 56Fe; measured not abstracted; deduced nuclear properties.


1962BA09      Bull.Am.Phys.Soc. 7, No.8, 572, F9 (1962)

J.B.Ball, C.B.Goodman, C.B.Fulmer

Nuclear Deformation of Mn55 Inferred from the Mn55(p, d) Reaction with 22-MeV Protons

NUCLEAR STRUCTURE 55Mn; measured not abstracted; deduced nuclear properties.


1962FU02      Bull.Am.Phys.Soc. 7, No.1, 83, Y8 (1962)

C.B.Fulmer, J.B.Ball, C.D.Goodman

(p, t) Reactions in Zirconium Isotopes

NUCLEAR STRUCTURE 91Nb, 92Zr, 89Zr, 90Zr, 94Zr; measured not abstracted; deduced nuclear properties.


1962GO01      Bull.Am.Phys.Soc. 7, No.1, 82, Y7 (1962)

C.D.Goodman, C.B.Fulmer, J.B.Ball

NUCLEAR STRUCTURE 88Y, 95Zr, 90Zr, 92Nb, 91Zr, 93Zr; measured not abstracted; deduced nuclear properties.


1962GO03      Bull.Am.Phys.Soc. 7, No.4, 316, MB6 (1962)

C.D.Goodman, J.B.Ball, C.B.Fulmer

Interpretations of Low-Lying Levels in Zirconium Isotopes Inferred from (p, p'), (p, d), and (p, t) Spectra

NUCLEAR STRUCTURE Zr; measured not abstracted; deduced nuclear properties.


1962GO16      Phys.Rev. 127, 574 (1962)

C.D.Goodman, J.B.Ball, C.B.Fulmer

Single-Particle Neutron Bound States in Iron Isotopes and in Cobalt Studied with (p, d) Reactions

NUCLEAR STRUCTURE 58Co, 57Fe, 56Fe, 53Fe, 55Fe; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.574
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1021.


1961BA01      Bull.Am.Phys.Soc. 6, No.1, 47, Q6 (1961)

J.B.Ball, C.D.Goodman, C.B.Fulmer

Single-Particle Neutron Bound States Near N = 28 Studied with (p, d) Reactions

NUCLEAR STRUCTURE 58Fe, 58Co, 57Fe, 56Fe, 55Fe, 53Fe; measured not abstracted; deduced nuclear properties.


1961FU02      Bull.Am.Phys.Soc. 6, No.3, 272, NA2 (1961)

C.B.Fulmer, C.D.Goodman, J.B.Ball

Deuteron Spectra from the Ni64(p, d)Ni63 Reaction

NUCLEAR STRUCTURE 63Ni; measured not abstracted; deduced nuclear properties.


1961GO33      Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.523 (1961)

C.D.Goodman, J.B.Ball, C.B.Fulmer

Pickup Reaction Studies of Neutron Bound States: Fe54 and Co59

NUCLEAR STRUCTURE 54Fe, 59Co; measured not abstracted; deduced nuclear properties.


1961GO34      Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.525 (1961)

C.D.Goodman, J.B.Ball, C.B.Fulmer

Pickup Reaction Evidence for Deformation of Fe56, Fe57, and Fe58

NUCLEAR STRUCTURE 57Fe, 56Fe, 55Fe; measured not abstracted; deduced nuclear properties.


1960BA12      Bull.Am.Phys.Soc. 5, No.4, 249, I12 (1960)

J.B.Ball

(p, t) Differential Cross Sections at 22 MeV

NUCLEAR STRUCTURE 49V, Rh, Nb, Co, V, Au; measured not abstracted; deduced nuclear properties.


1960BA39      Phys.Rev. 120, 488 (1960)

J.B.Ball, C.D.Goodman

Experimental Study of the Mechanism of (p, t) Reactions at 22 MeV

NUCLEAR STRUCTURE 197Au, 51V, 59Co, 92Zr, 93Nb, 90Zr, 91Zr, 103Rh, 101Ru; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.120.488
Citations: PlumX Metrics


1960GO10      Phys.Rev. 118, 1062 (1960)

C.D.Goodman, J.B.Ball

Survey of (p, d) Reactions at 22 MeV

NUCLEAR STRUCTURE 90Zr, 89Y, 93Nb, 92Zr, 92Nb, 91Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.118.1062
Citations: PlumX Metrics


1959BA32      Phys.Rev. 114, 305 (1959)

J.B.Ball, A.W.Fairhall, I.Halpern

Radiative Alpha-Particle Capture in Ni58 and Xe136 at Higher Energies

doi: 10.1103/PhysRev.114.305
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetP0072.


1958BA59      Bull.Am.Phys.Soc. 3, No.5, 322, H6 (1958)

J.B.Ball, A.W.Fairhall, I.Halpern

Capture Cross Sections for Moderate Energy Charged Particles


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