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Search: Author = J.L.Ford

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1988BE41      Phys.Scr. 38, 657 (1988)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson, G.A.Leander, C.W.Reich

Coulomb Excitation of States in 229Th

NUCLEAR REACTIONS 229Th(α, α), (α, α'), E=17 MeV; measured σ(Eα), σ(Eα') following Coulomb excitation. 229Th levels deduced excitation probability, B(E2), intrinsic quadrupole, hexadecapole moments, J, π, K, Nilsson assignments.

doi: 10.1088/0031-8949/38/5/004
Citations: PlumX Metrics


1988BU15      Phys.Rev. C38, 1680 (1988)

B.L.Burks, M.A.G.Fernandes, G.R.Satchler, D.J.Horen, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen

Optical Model and Coupled-Channels Analyses of the Elastic and Inelastic Scattering of 18O from 28Si at 352 MeV

NUCLEAR REACTIONS 28Si(18O, 18O), (18O, 18O'), E=351.7 MeV; measured σ(θ). Optical model, coupled-channels analyses.

doi: 10.1103/PhysRevC.38.1680
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1986FE03      Phys.Rev. C33, 1971 (1986)

M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen

One-Nucleon-Transfer Reactions Induced by 352-MeV 18O on 28Si

NUCLEAR REACTIONS 28Si(18O, 17O), (18O, 19F), E=352 MeV; measured σ(θ); deduced model parameters. 29Si, 27Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.

doi: 10.1103/PhysRevC.33.1971
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1986HO27      Phys.Lett. 181B, 38 (1986)

D.J.Horen, B.L.Burks, M.A.G.Fernandes, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, G.R.Satchler, D.Shapira, T.P.Sjoreen, F.Petrovich

Investigation of the One-Step Direct Contribution to the 28Si(18O, 18F)28Al Reaction at 19.6 MeV/Nucleon

NUCLEAR REACTIONS, MECPD 28Si(18O, 18F), E=352 MeV; measured σ(E(18F)), σ(θ); deduced reaction mechanism. Magnetic spectrometer system, particle identification ionization chamber. Microscopic DWIA calculations.

doi: 10.1016/0370-2693(86)91250-5
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1985SH06      Nucl.Instrum.Methods 228, 259 (1985)

D.Shapira, J.L.C.Ford, Jr., R.Novotny, B.Shivakumar, R.L.Parks, S.T.Thornton

The HHIRF Supersonic Gas Jet Target Facility

NUCLEAR REACTIONS 40Ar(16O, 16O), E=100 MeV; measured σ(θ). 40Ar(16O, 17O), E=100 MeV; measured σ(E(17O)). Supersonic gas jet target.

doi: 10.1016/0168-9002(85)90267-0
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1985SH30      Nucl.Instrum.Methods Phys.Res. B10/11, 436 (1985)

D.Shapira, J.Gomez del Campo, J.L.C.Ford, Jr., B.Shivakumar, P.H.Stelson, B.A.Harmon, R.L.Parks, S.T.Thornton

Nuclear Physics Experiments with the ORNL-HHIRF Supersonic Gas Jet Target

NUCLEAR REACTIONS 14N(28Si, X), E=150 MeV; measured fragment spectra; deduced orbiting process products mass, charge distribution features.

doi: 10.1016/0168-583X(85)90285-X
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1984GR02      Phys.Rev. C29, 459 (1984)

E.E.Gross, T.P.Cleary, J.L.C.Ford, Jr., D.C.Hensley, K.S.Toth, F.T.Baker, A.Scott, C.R.Bingham, J.A.Vrba

Nuclear Moments of the First Excited State of 22Ne from 22Ne(132 MeV) + 208Pb Scattering

NUCLEAR REACTIONS 208Pb(22Ne, 22Ne), (22Ne, 22Ne'), E=132 MeV; measured σ(θ); deduced optical potential parameters. 22Ne levels deduced quadrupole, hexadecapole deformation parameters, transition matrix elements. Enriched target, coupled-channels analysis.

doi: 10.1103/PhysRevC.29.459
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1984MA06      Phys.Rev.Lett. 52, 743 (1984)

C.F.Maguire, G.L.Bomar, M.E.Barclay, R.B.Piercey, A.V.Ramayya, J.L.C.Ford, Jr., D.Shapira, E.R.Flynn, J.D.Moses, J.C.Peng, N.Stein

Systematic Spectroscopic-Factor Discrepancy in Heavy-Ion Proton-Pickup Reactions on 40Ca

NUCLEAR REACTIONS 40Ca(10B, 11C), E=31 MeV; 40Ca(14C, 15N), E=41 MeV; measured σ(θ); deduced optical model parameters. 39K levels deduced spectroscopic factor reaction dependence. DWBA analysis, other data input.

doi: 10.1103/PhysRevLett.52.743
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1984SH19      Phys.Rev.Lett. 53, 1634 (1984)

D.Shapira, D.Schull, J.L.C.Ford, Jr., B.Shivakumar, R.L.Parks, R.A.Cecil, S.T.Thornton

Observation of Angular Momentum Saturation in Deep-Inelastic Processes involving Light Heavy Ions

NUCLEAR REACTIONS 12C(28Si, X), E=100-190 MeV; measured recoil projectile like fragment spectra; deduced fragment total kinetic energy vs E, angular momentum saturation.

doi: 10.1103/PhysRevLett.53.1634
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1983SH25      Phys.Rev. C28, 1148 (1983)

D.Shapira, D.DiGregorio, J.Gomez del Campo, R.A.Dayras, J.L.C.Ford, Jr., A.H.Snell, P.H.Stelson, R.G.Stokstad, F.Pougheon

Fusion and Peripheral Processes in the Collisions of 20Ne + 20Ne and 20Ne + 16O

NUCLEAR REACTIONS, ICPND 20Ne, 16O(20Ne, 20Ne), (20Ne, X), E=80-160 MeV; measured elastic σ, σ(fragment θ, E), σ(θ) for Z=6, 7, 8, 9, fusion σ(E), reaction σ, deep inelastic σ; deduced fusion potential parameters, entrance channel effects. Monte Carlo simulation.

doi: 10.1103/PhysRevC.28.1148
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1982BE12      Phys.Rev. C25, 1637 (1982)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Coulomb Excitation of Ground Band Rotational States in 249Bk

NUCLEAR REACTIONS 249Bk(α, α), (α, α'), E=17.06 MeV; measured σ(Eα, θ=150°). 249Bk levels deduced B(E2), B(M1), quadrupole moment, μ. Enriched target.

doi: 10.1103/PhysRevC.25.1637
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1982CH07      Phys.Rev. C25, 1410 (1982)

Y.-D.Chan, D.E.DiGregorio, J.L.C.Ford, Jr., J.Gomez del Campo, M.E.Oritz, D.Shapira

10B + 17O Fusion Cross Sections

NUCLEAR REACTIONS, ICPND 10B(17O, X), E=54, 72, 104, 124 MeV; measured σ(fragment θ, E) for Z=3-12; deduced fusion σ, critical (L), critical (J). Compound nucleus, statistical yrast limitation calculations.

doi: 10.1103/PhysRevC.25.1410
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1982DI13      Phys.Rev. C26, 1490 (1982)

D.E.DiGregorio, J.Gomez del Campo, Y.D.Chan, J.L.C.Ford, Jr., D.Shapira, M.E.Ortiz

14N + 13C Fusion Cross Sections and Compound Nucleus Limitation in 27Al

NUCLEAR REACTIONS, ICPND 13C(14N, X), E=86, 103.8, 149, 161.3, 180 MeV; measured σ(fragment θ, E) for fragment Z=5-12; deduced fusion, direct, reaction σ. 27Al deduced maximum J limit.

doi: 10.1103/PhysRevC.26.1490
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1982NO12      Phys.Rev. C26, 2664 (1982)

R.Novotny, D.Shapira, Y.-d.Chan, D.E.DiGregorio, J.L.C.Ford, Jr., J.Gomez del Campo, M.E.Ortiz, F.Pougheon

Fusion Cross Sections for the 12C + 15N System

NUCLEAR REACTIONS, ICPND 15N(12C, X), E=98, 117 MeV; measured σ(fragment θ, E); deduced fusion σ, evaporation residue relative yield, fusion mechanism. 27Al deduced J(critical). Glas-Mosel model.

doi: 10.1103/PhysRevC.26.2664
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1982OR02      Phys.Rev. C25, 1436 (1982)

M.E.Ortiz, J.Gomez del Campo, Y.D.Chan, D.E.DiGregorio, J.L.C.Ford, D.Shapira, R.G.Stokstad, J.P.F.Sellschop, R.L.Parks, D.Weiser

Fusion, Direct, and Total Reaction Cross Sections of the 10B + 14N System up to E(14N) = 180 MeV

NUCLEAR REACTIONS, ICPND 10B(14N, X), E=86-180 MeV; measured σ(fragment θ, E) for Z=3-11; deduced fusion σ, total σ, direct σ, grazing (L), critical (J) vs E. Optical, entrance channel model analyses.

doi: 10.1103/PhysRevC.25.1436
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1982SH16      Phys.Lett. 114B, 111 (1982)

D.Shapira, R.Novotny, Y.D.Chan, K.A.Erb, J.L.C.Ford, Jr., J.C.Peng, J.D.Moses

Deep-Inelastic Back-Angle Yields and Orbiting in 28Si + 12C

NUCLEAR REACTIONS, ICPND 12C(28Si, 12C), (28Si, 14N), (28Si, 16O), E=99-133 MeV; measured reaction σ, σ(E(12C)), σ(E(14N)), σ(E(16O)); deduced orbiting effect.

doi: 10.1016/0370-2693(82)90126-5
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1982SH29      Phys.Rev. C26, 2470 (1982)

D.Shapira, J.L.C.Ford, Jr., J.Gomez del Campo

Reactions of 20Ne with 12C

NUCLEAR REACTIONS, ICPND 12C(20Ne, 20Ne), (20Ne, 20Ne'), E=54-81 MeV; measured σ(θ) vs E; deduced reaction σ, reaction mechanism. 12C(20Ne, 16O), (20Ne, 12C), E=54-81 MeV; measured σ(θ) vs E; deduced reaction mechanism. DWBA, strong absorption, Monte Carlo statistical model.

doi: 10.1103/PhysRevC.26.2470
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1981BE54      Phys.Rev. C24, 2723 (1981)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Coulomb Excitation of Rotational States and Ground-State Quadrupole Moment for 243Am

NUCLEAR REACTIONS 243Am(α, α'), E=17 MeV; measured σ(Eα', θ=150°), Coulomb excitation. 243Am levels deduced B(E2), B(E4), quadrupole moment. Enriched target.

doi: 10.1103/PhysRevC.24.2723
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1981DE09      Nucl.Phys. A357, 521 (1981)

L.C.Dennis, K.R.Cordell, R.R.Doering, R.L.Parks, S.T.Thornton, J.L.C.Ford, Jr., J.Gomez Del Campo, D.Shapira

Search for Resonances in 12C(9Be, α)17O

NUCLEAR REACTIONS 12C(9Be, α), E=9-20 MeV; measured σ(E, θ); 12C(9Be, α), E=16.1, 17, 17.9 MeV; measured σ(θ). Natural targets. Hauser-Feshbach calculations, compound plus resonance, compound plus direct mechanisms.

doi: 10.1016/0375-9474(81)90234-7
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1980FO02      Phys.Rev. C21, 764 (1980)

J.L.C.Ford, Jr., T.P.Cleary, J.Gomez del Campo, D.C.Hensley, D.Shapira, K.S.Toth

First 8+ State in 28Si and Level Systematics of sd Shell Nuclei

NUCLEAR REACTIONS 25Mg(12C, 9Be), E=100, 120 MeV; measured σ(θ). 28Si deduced levels, J, π. Shell model calculations, DWBA analysis.

doi: 10.1103/PhysRevC.21.764
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1980MA31      Phys.Rev. C22, 1097 (1980)

C.F.Maguire, G.L.Bomar, A.V.Ramayya, R.B.Piercey, J.L.C.Ford, Jr., J.G.del Campo, D.Shapira, D.Hensley

Comparison of the Single-Proton Pickup Reactions 40Ca(11B, 12C)39K and 40Ca(13C, 14N)39K at Low and High Bombarding Energies

NUCLEAR REACTIONS 40Ca(11B, 12C), E=32, 68 MeV; 40Ca(13C, 14N), E=40, 68 MEV; 40Ca(11B, 11B), E=32 MeV; measured σ(θ); deduced optical model parameters. 39K levels deduced S. DWBA analysis.

doi: 10.1103/PhysRevC.22.1097
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1980OR03      Phys.Rev. C22, 1104 (1980)

M.E.Ortiz, E.Andrade, M.Cardenas, A.Dacal, A.Menchaca-Rocha, J.L.C.Ford, Jr., J.G.del Campo, R.L.Robinson, D.Shapira, E.Aguilera

Nonstatistical Effects in the 12C(15N, α) Reaction

NUCLEAR REACTIONS 12C(15N, α), E=21.4-39 MeV; 12C(15N, 15N), E=22-31.8 MEV; measured σ(E, θ); deduced nonstatistical effects. 27Al deduced high-spin resonances. Hauser-Feshbach formalism, fluctuation, single-level analysis.

doi: 10.1103/PhysRevC.22.1104
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1980SH10      Phys.Rev. C21, 1824 (1980)

D.Shapira, J.L.C.Ford, Jr., J.Gomez del Campo, P.H.Stelson

Backward Angle Cross Sections for 27Al + 16O Reaction Products

NUCLEAR REACTIONS 16O(27Al, X), E=105, 145 MeV; measured σ(θ); deduced evaporation residue, damped event σ.

doi: 10.1103/PhysRevC.21.1824
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1979BA19      Nucl.Phys. A321, 222 (1979)

F.T.Baker, A.Scott, T.P.Cleary, J.L.C.Ford, E.E.Gross, D.C.Hensley

194Pt(12C, 12C') Reaction and the Triaxial-Rotor Model

NUCLEAR REACTIONS 194Pt(12C, 12C'), E=78 MeV, θ(cm)=25°-80°; measured σ(E(12C), θcm). 194Pt deduced optical-model parameters, asymmetric-rotor model parameters β2, β4, γ. Enriched target.

doi: 10.1016/0375-9474(79)90695-X
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1979CL05      Phys.Lett. 83B, 51 (1979)

T.P.Cleary, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, C.R.Bingham, J.A.Vrba

Mutual Excitation of 22Ne and 126Te in Inelastic Scattering

NUCLEAR REACTIONS 126Te(22Ne, 22Ne'), E=93.5 MeV; measured σ(θ) for mutual excitation. 126Te, 22Ne levels deduced static quadrupole moment, B(E2). Enriched target. Coupled-channel analysis.

doi: 10.1016/0370-2693(79)90886-4
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1979CO11      Nucl.Phys. A323, 147 (1979)

K.R.Cordell, S.T.Thornton, L.C.Dennis, P.G.Lookadoo, T.C.Schweizer, J.L.C.Ford, Jr., J.Gomez del Campo, D.Shapira

The 12C(13C, α)21Ne Reaction: High-Spin States, Resonances and Coherence Widths

NUCLEAR REACTIONS 12C(13C, α), E=18.2-32.0 MeV; measured σ(E). 12C(13C, α), E=29-31 MeV; measured σ(θ). 21Ne deduced levels, J, π. 25Mg deduced coherence width, moment of inertia.

doi: 10.1016/0375-9474(79)90420-2
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1979FO22      Phys.Lett. 89B, 48 (1979)

J.L.C.Ford, Jr., J.Gomez del Campo, D.Shapira, M.R.Clover, R.M.DeVries, B.R.Fulton, R.Ost, C.F.Maguire

Systematics of Back Angle 12C Scattering - The 12C + 20Ne and 12C + 24Mg Systems

NUCLEAR REACTIONS 12C(20Ne, 12C), E=55-80 MeV; 12C(24Mg, 12C), E(cm)=17-30 MeV; measured σ(E, θ). Legendre polynomial analysis.

doi: 10.1016/0370-2693(79)90073-X
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1979MC04      Phys.Rev. C20, 2093 (1979)

F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, D.Shapira, P.H.Stelson

Coulomb Excitation of 183W

NUCLEAR REACTIONS 183W(α, α'γ), E=15 MeV; 183W(α, α'), E=13 MeV; measured Eγ, Iγ, γ(θ), σ(Eα'; θ). 183W levels deduced B(E2), B(M1), J, π, δ. Enriched targets.

doi: 10.1103/PhysRevC.20.2093
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1979SH18      Phys.Rev.Lett. 43, 1781 (1979)

D.Shapira, J.L.C.Ford, Jr., J.Gomez del Campo, R.G.Stokstad, R.M.DeVries

Orbiting in the 12C + 20Ne System

NUCLEAR REACTIONS 12C(20Ne, 11C), (20Ne, 13C), (20Ne, 16O), (20Ne, 20Ne'), E=50-80 MeV; measured σ(E, θ); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.43.1781
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1979SH22      Nucl.Instrum.Methods 163, 325 (1979)

D.Shapira, R.Dayras, J.L.C.Ford, Jr., J.Gomez del Campo, A.H.Snell, P.H.Stelson, R.G.Stokstad

A Gas Cell Target for Studying Fusion and Damped Collisions of Light Nuclei

NUCLEAR REACTIONS 20Ne(20Ne, X), E(cm)=83 MeV; measured fusion σ(θ). 16O(20Ne, X), E=131 MeV; measured evaporation residue energy for 12C, 14N, 16O, 19F, 20Ne, 23Na, 24Mg, 27Al, 28Si, 31P, 32S.

doi: 10.1016/0029-554X(79)90115-0
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1978CO04      Nucl.Phys. A296, 278 (1978)

K.R.Cordell, S.T.Thornton, L.C.Dennis, T.C.Schweizer, J.Gomez del Campo, J.L.C.Ford, Jr.

Statistical Model Analysis of the 12C(14N, α) Reaction and Coherence Widths in 26Al

NUCLEAR REACTIONS 12C(14N, α), E=22-39.2 MeV; measured σ(E). 26Al deduced average coherence Γ, moment of inertia. Hauser-Feshbach calculations.

doi: 10.1016/0375-9474(78)90073-8
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1978GO06      Nucl.Phys. A297, 125 (1978)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, M.E.Ortiz, A.Dacal, E.Andrade

Coherence Widths in 27Al Measured with the 12C(15N, α) Reaction

NUCLEAR REACTIONS 12C(15N, α), E=21.4-39.0 MeV; measured σ(E) at θ=7°. 27Al deduced coherence widths, effective moment of inertia. Hauser-Feshbach analysis.

doi: 10.1016/0375-9474(78)90202-6
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1978GR06      Phys.Rev. C17, 1665 (1978)

E.E.Gross, T.P.Cleary, J.L.C.Ford, D.C.Hensley, K.S.Toth

20Ne Nuclear Moments from 20Ne(131 MeV) + 208Pb Scattering

NUCLEAR REACTIONS 208Pb(20Ne, 20Ne), (20Ne, 20Ne'), E=131 MeV; measured σ(θ); deduced optical potential. 20Ne level deduced β(L), quadrupole moment, B(E2).

doi: 10.1103/PhysRevC.17.1665
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1978TH01      Phys.Rev. C17, 576 (1978)

S.T.Thornton, D.E.Gustafson, K.R.Cordell, L.C.Dennis, T.C.Schweizer, J.L.C.Ford, Jr.

Levels in 23Na Populated by the 12C(15N, α) Reaction

NUCLEAR REACTIONS 12C(15N, α), E=36.0-39.2 MeV; measured σ(E, θ). 23Na deduced levels, K, J, π. Hauser-Feshbach analysis, natural target.

doi: 10.1103/PhysRevC.17.576
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1977GO08      Phys.Lett. 69B, 415 (1977)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, M.E.Ortiz, A.Dacal, E.Andrade

Yrast Levels in 27Al Suggested by Resonance Structure in the 12C(15N, α) Reaction

NUCLEAR REACTIONS 12C(15N, α), E=21.4-39.0 MeV; measured σ(E, Eα). 27Al deduced resonances.

doi: 10.1016/0370-2693(77)90833-4
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1977RE08      Nucl.Phys. A283, 149 (1977)

H.Reiss, H.V.Klapdor, G.Rosner, J.L.C.Ford, Jr., S.T.Thornton

Enhanced 9Be Production in the 14N + 11B Reaction

NUCLEAR REACTIONS 11B(14N, 9Be), E=50 MeV; measured σ(E(9Be), θ). Hauser-Feshbach analysis.

doi: 10.1016/0375-9474(77)90704-7
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1977RO08      Phys.Rev. C15, 1671 (1977)

R.M.Ronningen, J.H.Hamilton, A.V.Ramayya, L.Varnell, G.Garcia-Bermudez, J.Lange, W.Lourens, L.L.Riedinger, R.L.Robinson, P.H.Stelson, J.L.C.Ford, Jr.

Reduced Transition Probabilities of Vibrational States in 154-160Gd and 176-180Hf

NUCLEAR REACTIONS 154,156,158,160Gd, 176,178,180Hf(α, α'), E=11-17 MeV; measured σ(E, Eα', θ), Coulomb excitation. 154,156,158,160Gd, 176,178,180Hf levels deduced B(λ), M(λ). Enriched targets.

doi: 10.1103/PhysRevC.15.1671
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1977RO26      Phys.Rev. C16, 2208 (1977)

R.M.Ronningen, J.H.Hamilton, L.Varnell, J.Lange, A.V.Ramayya, G.Garcia-Bermudez, W.Lourens, L.L.Riedinger, F.K.McGowan, P.H.Stelson, R.L.Robinson, J.L.C.Ford, Jr.

E2 and E4 Reduced Matrix Elements of 154,156,158,160Gd and 176,178,180Hf

NUCLEAR REACTIONS 154,156,158,160Gd, 176,178,180Hf(α, α'), E=11.5-14 MeV; measured Coulomb excitation σ(E). 154,156,158,160Gd, 176,178,180Hf levels deduced β2, β4.

doi: 10.1103/PhysRevC.16.2208
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1977WA11      Phys.Rev. C16, 1271 (1977)

G.J.Wagner, K.T.Knopfle, G.Mairle, P.Doll, H.Hafner, J.L.C.Ford, Jr.

Strong Effect of Isospin Mixing in 16O

NUCLEAR REACTIONS 17O(d, 3He), (d, t), E=52 MeV; 17O(3He, α), E=36 MeV; measured σ(θ); deduced relative population of states. 16O levels deduced T-mixing.

doi: 10.1103/PhysRevC.16.1271
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1976FR02      Nucl.Phys. A256, 93 (1976)

E.Friedland, M.Goldschmidt, C.A.Wiedner, J.L.C.Ford, Jr., S.T.Thornton

Spectroscopic Investigation of the 144Sm(3He, α)143Sm Reaction

NUCLEAR REACTIONS 144Sm(3He, α), (3He, 3He), E=30 MeV; measured σ(θ). 143Sm deduced levels, L, J, π, spectroscopic factors. Enriched target, θ=10-70°, Δθ=2.6°.

doi: 10.1016/0375-9474(76)90096-8
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1976GO07      Nucl.Phys. A262, 125 (1976)

J.Gomez del Campo, M.E.Ortiz, A.Dacal, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the Coherence Widths Γ in 28Si Measured by the 12C(16O, α) Reaction

NUCLEAR REACTIONS 12C(16O, α), E=40-46 MeV; measured σ(E) for θ=7°. 24Mg levels deduced Γ. 28Si deduced coherence widths. Hauser-Feshbach calculations, fluctuation analysis.

doi: 10.1016/0375-9474(76)90444-9
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1976GU05      Phys.Rev. C13, 691 (1976)

D.E.Gustafson, S.T.Thornton, T.C.Schweizer, J.L.C.Ford, Jr., P.D.Miller, R.L.Robinson, P.H.Stelson

High-Spin States of the Kπ = 3/2+ and 1/2+ Bands of 23Na

NUCLEAR REACTIONS 12C(15N, α), E=36-39.2 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π, K. Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.13.691
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1976TH04      Phys.Rev. C13, 1502 (1976)

S.T.Thornton, D.E.Gustafson, J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley

Inelastic Scattering and Transfer Reactions from 12C Ions on 90Zr

NUCLEAR REACTIONS 90Zr(12C, 12C), (12C, 11C), (12C, 11B), E=98 MeV; measured σ(θ); deduced optical model parameters. 90Zr deduced β. 91Zr, 91Nb levels deduced S.

doi: 10.1103/PhysRevC.13.1502
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1976TH05      Phys.Rev. C13, 1936 (1976)

S.T.Thornton, T.C.Schweizer, D.E.Gustafson, J.L.C.Ford, Jr., M.J.LeVine

Nuclear Structure Study of 141Nd, 143Nd, and 143Pm by 13C-Induced Reactions on 142Nd

NUCLEAR REACTIONS 142Nd(13C, 14C), (13C, 12C), (13C, 12B), E=67.5 MeV; measured σ(θ). 141,143Nd, 143Pm levels deduced L, J, π, S. DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.13.1936
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1976TH15      Nucl.Phys. A270, 428 (1976)

S.T.Thornton, T.C.Schweizer, D.E.Gustafson, J.L.C.Ford, Jr., M.J.Levine

Nuclear and Coulomb Deformation Parameters of 142Nd

NUCLEAR REACTIONS 142Nd(13C, 13C), (13C, 13C'), E=67.5 MeV; measured σ(E, θ). 142Nd levels deduced β(L), DWBA analyses. Enriched target. Resolution 70 keV; θ lab=20-75°, Δθ=1°.

doi: 10.1016/0375-9474(76)90455-3
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1976TO08      Phys.Rev. C14, 1471 (1976)

K.S.Toth, J.L.C.Ford, Jr., G.R.Satchler, E.E.Gross, D.C.Hensley, S.T.Thornton, T.C.Schweizer

Measurements and Analysis of the 208Pb(12C, 13C), (12C, 11B), and (12C, 14C) Reactions

NUCLEAR REACTIONS 208Pb(12C, 13C), (12C, 11B), E=77.4, 97.9, 116.4 MeV; 208Pb(12C, 14C), E=97.9 MeV; 207Pb(13C, 13C), E=86.1 MeV; 209Bi(11B, 11B), E=74.6 MeV; measured σ(θ). 209Bi, 207Pb levels deduced S. Optical model, DWBA analysis.

doi: 10.1103/PhysRevC.14.1471
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1976WE14      Phys.Rev. C13, 2588 (1976)

J.C.Wells, Jr., R.L.Robinson, H.J.Kim, J.L.C.Ford, Jr.

Absolute Cross Sections for the 61Ni(16O, 3n)74Kr Reaction

NUCLEAR REACTIONS 61Ni(16O, 3n), E=38.5-51.0 MeV; measured nothing, reanalyzed data; deduced σ(E).

doi: 10.1103/PhysRevC.13.2588
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1975LE22      Phys.Rev. C12, 1483 (1975)

I.Y.Lee, J.X.Saladin, J.Holden, J.O'Brien, C.Baktash, C.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle

Deformation Parameters of the Charge Distribution and the Optical Potential for Some Nuclei in and Near the Rare Earth Region

NUCLEAR REACTIONS 154Sm(α, α'), E=11-19 MeV; 166Er(α, α'), E=12.5-19.5 MeV; 182W(α, α'), E=13-21 MeV; measured σ(Eα'). 168Er(α, α'), E=13-19 MeV; 184W(α, α'), E=12.5-19 MeV; 186W(α, α'), E=13.25-19 MeV; measured σ(Eα', θ). 154Sm, 166,168Er, 182,184,186W deduced M(E2), M(E4), charge deformations, optical potential deformations.

doi: 10.1103/PhysRevC.12.1483
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1975SA17      Phys.Lett. 60B, 43 (1975)

G.R.Satchler, J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley, E.E.Gross, D.E.Gustafson, S.T.Thornton

A Microscopic Description of Inelastic 12C Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(12C, 12C'), E=98 MeV; measured σ(E(12C'), θ). 208Pb deduced levels, J.

doi: 10.1016/0370-2693(75)90522-5
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1975TH09      Phys.Rev. C12, 877 (1975)

S.T.Thornton, J.L.C.Ford, Jr., E.Friedland, C.A.Wiedner, M.Goldschmidt

13C + 144Sm Neutron-Transfer Reaction

NUCLEAR REACTIONS 144Sm(13C, 13C), E=66 MeV; measured σ(θ); deduced optical model parameters. 144Sm(13C, 12C), E=66, 72 MeV; measured σ(E(12C), θ). 144Sm(13C, 14C), E=66, 72 MeV; measured σ(E(14C), θ). 143,145Sm levels deduced J, π, S.

doi: 10.1103/PhysRevC.12.877
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1975WE05      Phys.Rev. C11, 879 (1975)

J.C.Wells, Jr., R.L.Robinson, H.J.Kim, J.L.C.Ford, Jr.

Absolute Cross Sections for the 61Ni(16O, X) Reactions

NUCLEAR REACTIONS 61Ni(16O, X), E=38.5, 41.0, 43.5, 46.0, 48.5, 51.0 MeV; measured Eγ, Iγ; deduced σ(E).

doi: 10.1103/PhysRevC.11.879
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1975WE20      Phys.Rev. C12, 1529 (1975)

J.C.Wells, Jr., R.L.Robinson, H.J.Kim, J.L.C.Ford, Jr.

Absolute Cross Sections for the 63,65Cu(16O, X) Reactions

NUCLEAR REACTIONS 63,65Cu(16O, n), (16O, p), (16O, 2n), (16O, 2p), (16O, pn), 63,65Cu(16O, 3n), (16O, 2np), (16O, n2p), (16O, 3p), (16O, α), (16O, nα), (16O, pα), 63,65Cu(16O, 2nα), (16O, npα), (16O, 2α), (16O, 12C), (16O, 15N), (16O, 17F), 63Cu(16O, n2α), (16O, p2α), (16O, 14C), (16O, 14N), (16O, 14O), (16O, 15O), (16O, 18O), 63Cu(16O, 18F), E=38.5-51.0 MeV; measured Eγ, Iγ; deduced σ(E).

doi: 10.1103/PhysRevC.12.1529
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1974CO14      Phys.Rev. C9, 1457 (1974)

W.E.Collins, J.H.Hamilton, R.L.Robinson, H.J.Kim, J.L.C.Ford, Jr.

Levels in 72Se Populated by 72Br

RADIOACTIVITY 72Br; measured T1/2, Eγ, Iγ, γγ coin. 72Se deduced levels, J, π.

doi: 10.1103/PhysRevC.9.1457
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1974FO11      Nucl.Phys. A226, 189 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

States in 24Mg Populated by the 10B(16O, d)24Mg and 12C(16O, α)24Mg Reactions

NUCLEAR REACTIONS 10B(16O, d), E=44-46 MeV; 12C(16O, α), E=40-46 MeV; measured σ(E). 24Mg deduced levels, J.

doi: 10.1016/0375-9474(74)90401-1
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1974FO15      Z.Phys. 269, 147 (1974)

J.L.C.Ford, Jr., J.Gomez del Campo, R.L.Robinson, P.H.Stelson, S.T.Thornton

Measurements and Hauser-Feshbach Analysis of the 10B(16O, 6Li)20Ne Reaction

NUCLEAR REACTIONS 10B(16O, 6Li), E=44.4-46 MeV; measured σ(E, E(6Li)). 20Ne deduced levels. Hauser-Feshbach calculations.

doi: 10.1007/BF01669056
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1974FO22      Phys.Rev. C10, 1429 (1974)

J.L.C.Ford, Jr., K.S.Toth, G.R.Satchler, D.C.Hensley, L.W.Owen, R.M.DeVries, R.M.Gaedke, P.J.Riley, S.T.Thornton

Single-Nucleon Transfer Reactions Induced by 11B Ions on 208Pb: A test of the distorted-wave born approximation

NUCLEAR REACTIONS 208Pb(11B, 10B), (11B, 12B), (11B, 10Be), (11B, 12C), E=72.2 MeV; measured σ(E(10B), θ), σ(E(12B), θ), σ(E(10Be), θ), σ(E(12C), θ). 209,207Pb, 209Bi, 207Tl levels deduced S.

doi: 10.1103/PhysRevC.10.1429
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1974GO10      Phys.Rev. C9, 1258 (1974)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, S.T.Thornton

Study of the 10B(16O, α)22Na Reaction

NUCLEAR REACTIONS 10B(16O, α), E(16O)=40-46 MeV, measured σ(E) for θ(lab)=7°; E(16O)=46 MeV, measured σ(θ). 22Na deduced levels. Fluctuation analysis. Hauser-Feshbach calculations, suggested J values. Enriched targets.

doi: 10.1103/PhysRevC.9.1258
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1974MC15      Phys.Rev. C10, 1146 (1974)

F.K.McGowan, C.E.Bemis, Jr., W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson

Coulomb Excitation of Vibrational-Like States in the Even-A Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 236,238U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα'). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm levels deduced B(E2), B(E3). Enriched targets.

doi: 10.1103/PhysRevC.10.1146
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1974RO14      Phys.Rev. C9, 1402 (1974)

R.L.Robinson, H.J.Kim, J.L.C.Ford, Jr.

Absolute Cross Sections for the 58,60Ni(16O, X) Reactions

RADIOACTIVITY 68,69,70As, 66,68,69,72Ge, 71,73Se, 72Br, 74Kr, 66Ga, 62Zn; measured Eγ, Iγ. 74Br; measured Eγ, Iγ, T1/2.

NUCLEAR REACTIONS 58,60Ni(16O, X), E=38, 42, 46 MeV; measured Eγ, Iγ; deduced σ(E).

doi: 10.1103/PhysRevC.9.1402
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1973BE40      Phys.Rev. C8, 1934 (1973)

C.E.Bemis, Jr., P.H.Stelson, F.K.McGowan, W.T.Milner, J.L.C.Ford, Jr., R.L.Robinson, W.Tuttle

Interference between Direct Nuclear Reactions and Coulomb Excitation with Alpha Particles on 154Sm, 166Er, and 182W

NUCLEAR REACTIONS 154Sm, 166Er, 182W(α, α), (α, α'), E=11-21 MeV; measured σ(E;Eα'). 154Sm, 166Er levels deduced E2, E4 matrix elements.

doi: 10.1103/PhysRevC.8.1934
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1973BE44      Phys.Rev. C8, 1466 (1973)

C.E.Bemis, Jr., F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner, P.H.Stelson, R.L.Robinson

E2 and E4 Transition Moments and Equilibrium Deformations in the Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 236U(α, α'), E=16, 17 MeV; 234U(α, α'), E=16-19 MeV; 238U(α, α'), E=16-18 MeV; 238,240,242,244Pu, 244,246,248Cm(α, α'), E=17 MeV; measured σ(Eα', θ). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm deduced B(E2), B(E4), β.

doi: 10.1103/PhysRevC.8.1466
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1973DE12      Nucl.Phys. A204, 307 (1973)

J.A.Deye, R.L.Robinson, J.L.C.Ford, Jr.

The 110Pd, 116Cd(p, p'γ) Reactions

NUCLEAR REACTIONS 110Pd(p, p'γ), Ep=13 MeV; 116Cd(p, p'γ), Ep=12 MeV; measured σ(Ep', Eγ). 110Pd, 116Cd deduced levels, J, π, γ-branching. Enriched targets.

doi: 10.1016/0375-9474(73)90275-3
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1973FO17      Phys.Rev. C8, 1912 (1973)

J.L.C.Ford, Jr., K.S.Toth, D.C.Hensley, R.M.Gaedke, P.J.Riley, S.T.Thornton

Interference between Coulomb and Nuclear Excitation in the Inelastic Scattering of 11B Ions from 208Pb

NUCLEAR REACTIONS 208Pb(11B, 11B), (11B, 11B'), E=72.2 MeV; measured σ(θ). Studied Coulomb, nuclear interference. DWBA analysis. Enriched target.

doi: 10.1103/PhysRevC.8.1912
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1973GO32      Phys.Lett. 46B, 180 (1973)

J.Gomez del Campo, J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, J.B.McGrory, S.T.Thornton

Population of High Spin States in 22Na by Means of the 10B(16O, α) Reaction

NUCLEAR REACTIONS 10B(16O, α), E=46 MeV; measured σ(Eα, θ). 22Na deduced levels of high J.

doi: 10.1016/0370-2693(73)90677-1
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1972DE06      Nucl.Phys. A180, 449 (1972)

J.A.Deye, R.L.Robinson, J.L.C.Ford, Jr.

Elastic and Inelastic Proton Scattering from 116Cd

NUCLEAR REACTIONS 116Cd(p, p), (p, p'), Ep=12 MeV; measured σ(Ep, θ), σ(Ep', θ). 116Cd deduced levels, deformation parameters β(L). Enriched targets. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(72)90872-X
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1972FO02      Nucl.Instrum.Methods 98, 199 (1972)

J.L.C.Ford, Jr., P.H.Stelson, R.L.Robinson

A Position Sensitive Proportional Detector for a Magnetic Spectrograph

NUCLEAR REACTIONS 246Cm(α, α'), E=17 MeV; measured σ(Eα'). 246Cm deduced B(E2). 238U(α, α'), E=15 MeV; measured σ(Eα'). 238U deduced levels.

doi: 10.1016/0029-554X(72)90098-5
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1972HO28      Nucl.Phys. A190, 362 (1972)

J.L.Horton, C.L.Hollas, P.J.Riley, S.A.S.Zaidi, C.M.Jones, J.L.C.Ford, Jr.

The 90Zr(d, n)91Nb and 96Zr(d, n)97Nb Reactions

NUCLEAR REACTIONS 90Zr(d, n)91Nb, 96Zr(d, n)97Nb, E=12 MeV; measured σ(En, θ). 91Nb, 97Nb levels deduced angular momentum transfer values, S.

doi: 10.1016/0375-9474(72)90147-9
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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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1972RA32      Nucl.Phys. A193, 186 (1972)

A.V.Ramayya, J.L.C.Ford, Jr., R.L.Robinson, J.H.Hamilton

Elastic and Inelastic Proton Scattering from 86Sr

NUCLEAR REACTIONS 86Sr(p, p'), Ep=12 MeV; measured σ(θ). 86Sr deduced levels, deformation parameters. DWBA, coupled-channel calculations. Enriched target.

doi: 10.1016/0375-9474(72)90244-8
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1971FO17      Phys.Rev.Lett. 27, 1232 (1971)

J.L.C.Ford, Jr., P.H.Stelson, C.E.Bemis, Jr., F.K.McGowan, R.L.Robinson, W.T.Milner

Precise Coulomb Excitation B(E2) Values for First 2+ States of the Actinide Nuclei

NUCLEAR REACTIONS 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf(α, α'), E=17, 18 MeV; measured B(E2). 230,232Th, 234,236,238U, 238,240,242,244Pu, 244,246,248Cm, 252Cf deduced B(E2). 252Cf deduced level.

doi: 10.1103/PhysRevLett.27.1232
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1971MC21      Phys.Rev.Lett. 27, 1741 (1971)

F.K.McGowan, C.E.Bemis, Jr., J.L.C.Ford, Jr., W.T.Milner, R.L.Robinson, P.H.Stelson

Equilibrium Quadrupole and Hexadecapole Deformations in 230Th and 238U

NUCLEAR REACTIONS 230Th, 238U(α, α), (α, α'), E=17, 18 MeV; measured σ(Eα'). 230Th, 238U deduced B(EL), equilibrium deformation parameters.

doi: 10.1103/PhysRevLett.27.1741
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1971RA17      Nucl.Phys. A170, 199 (1971)

J.Rapaport, R.L.Robinson, J.L.C.Ford, Jr., M.N.Rao

Stripping Analysis of the 87Rb(d, p)88Rb Reaction

NUCLEAR REACTIONS 87Rb(d, p), E=11 MeV; measured Q, σ(Ep, θ). 88Rb deduced levels, L, J, π, transition strengths. Enriched targets.

doi: 10.1016/0375-9474(71)90693-2
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1971RI12      Phys.Rev. C4, 1864 (1971)

P.J.Riley, J.L.Horton, C.L.Hollas, S.A.A.Zaidi, C.M.Jones, J.L.C.Ford, Jr.

Spectroscopy of 93,95,97Tc through the (d, n) Reaction

NUCLEAR REACTIONS 92,94,96Mo(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc deduced levels, J, π, L(p), S.

doi: 10.1103/PhysRevC.4.1864
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1970DE26      Nucl.Phys.To Be Published (1970); See Also 70De25

J.A.Deye, R.L.Robinson, J.L.C.Ford, Jr.

The (p, p'γ) Reaction on 110Pd


1970FO01      Nucl.Phys. A142, 525 (1970)

J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson, T.Tamura, C.-Y.Wong

Elastic and Inelastic Proton Scattering from 109Ag

NUCLEAR REACTIONS 109Ag(p, p'), E=13 MeV; measured σ(θ). 109Ag deduced levels, deformation parameters. Enriched target.

doi: 10.1016/0375-9474(70)90810-9
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1970JO25      Phys.Rev. C2, 2113 (1970)

C.M.Jones, J.L.C.Ford, Jr., F.E.Obenshain, M.Reeves III

Search for Parity Nonconservation in the Force between Nucleons

RADIOACTIVITY 16N; measured β-delayed α-spectrum. 16O level deduced no parity-forbidden α-decay.

doi: 10.1103/PhysRevC.2.2113
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1970RA13      Nucl.Phys. A147, 1 (1970)

M.N.Rao, P.H.Stelson, R.L.Robinson, J.L.C.Ford, Jr.

Elastic and Inelastic Proton Scattering from 124Te

NUCLEAR REACTIONS 124Te(p, p), (p, p'), E = 12 MeV; measured σ(Ep, θ), σ(Ep', θ). 124Te deduced levels, deformation parameters β(L). Enriched target. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(70)90504-X
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1970ZA09      Phys.Rev.Lett. 25, 1503 (1970)

S.A.A.Zaidi, C.L.Hollas, J.L.Horton, P.J.Riley, J.L.C.Ford, Jr., C.M.Jones

Anomalies in the Cross Sections of (d, n) Reactions Leading to Isobaric Analog States

NUCLEAR REACTIONS 92,94,96Mo, 96Zr(d, n), E=12 MeV; measured σ(En, θ). 93,95,97Tc, 97Nb deduced isobaric analog states, S.

doi: 10.1103/PhysRevLett.25.1503
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1969RO30      Phys.Rev. 187, 1609 (1969)

R.L.Robinson, J.L.C.Ford, Jr., P.H.Stelson, T.Tamura, C.Y.Wong

Elastic and Inelastic Proton Scattering from 110Pd

NUCLEAR REACTIONS 110Pd(p, p), (p, p'), E=13 MeV; measured σ(Ep', θ). 110Pd deduced levels, J, π, β(L).

doi: 10.1103/PhysRev.187.1609
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1968CZ01      Phys.Rev. 174, 331 (1968)

G.Czjzek, J.L.C.Ford, Jr., J.C.Love, F.E.Obenshain, H.H.F.Wegener

Coulomb-Recoil-Implantation Mossbauer Experiments with 73Ge

NUCLEAR REACTIONS 73Ge(16O, 16O'γ), E=25 MeV; measured Mossbauer effect for 73Ge recoils into Cr, Fe, Cu, Ge. 73Ge levels deduced J, T1/2, isomer shift in GeO2.

doi: 10.1103/PhysRev.174.331
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1968ST18      Nucl.Phys. A119, 14 (1968)

P.H.Stelson, J.L.C.Ford, Jr., R.L.Robinson, C.Y.Wong, T.Tamura

Elastic and Inelastic Proton Scattering from 112,114Cd

NUCLEAR REACTIONS 112,114Cd(p, p), (p, p'), E=13 MeV; measured σ(Ep, θ), σ(Ep', θ). 112,114Cd deduced levels, deformation parameters β(L). Enriched targets. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(68)90802-6
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1967CZ01      Phys.Rev.Letters 18, 529 (1967)

G.Czjzek, J.L.C.Ford, Jr., J.C.Love, F.E.Obenshain, H.H.F.Wegener

Coulomb-Recoil-Implantation Mossbauer Experiments with 73Ge

NUCLEAR STRUCTURE 73Ge; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.18.529
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1967FO03      Bull.Am.Phys.Soc. 12, No.1, 128, HF2 (1967)

J.L.C.Ford, Jr., K.L.Warsh, R.L.Robinson, C.D.Moak

63,65Cu(3He, D)64,66Zn Reactions

NUCLEAR STRUCTURE 64Zn, 66Zn; measured not abstracted; deduced nuclear properties.


1967FO06      ORNL-4082, p.42 (1967)

J.L.C.Ford, Jr., K.L.Warsh, R.L.Robinson, C.D.Moak

The 65Cu(3He, D)66Zn reaction

NUCLEAR STRUCTURE 66Zn; measured not abstracted; deduced nuclear properties.


1967FO08      Phys.Rev. 158, 1194 (1967)

J.L.C.Ford, Jr., C.-Y.Wong, T.Tamura, R.L.Robinson, P.H.Stelson

Elastic and Inelastic Proton Scattering from 107Ag and the Phonon-Core Model

NUCLEAR STRUCTURE 107Ag; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.158.1194
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1967FO10      Nucl.Phys. A103, 525 (1967)

J.L.C.Ford, Jr., K.L.Warsh, R.L.Robinson, C.D.Moak

The 63,65Cu(3He, d)64,66Zn Reactions

NUCLEAR REACTIONS 63,65Cu(3He, d), E=18 MeV; measured σ(E, θ). 64,66Zn deduced levels, L, S. Enriched targets.

doi: 10.1016/0375-9474(67)90921-9
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1966BA03      Phys.Rev. 144, 799 (1966)

J.K.Bair, J.L.C.Ford, Jr., C.M.Jones

Total Neutron Yield from the Reaction 14C(α, n)17O

NUCLEAR STRUCTURE 14C, 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.144.799
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1966CZ01      Phys.Letters 19, 673 (1966)

G.Czjzek, J.L.C.Ford, Jr., F.E.Obenshain, D.Seyboth

Observation of the Mossbauer Effect following Coulomb Excitation of 73Ge

NUCLEAR STRUCTURE 73Ge; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90437-9
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1966MC18      Proc.Conf.Bases for Nucl.Spin-Parity Assignments, Gatlinburg, Tenn. (1966), N.B.Gove, R.L.Robinson, Eds., Academic Press, New York, p.222 (1966)

F.K.McGowan, P.H.Stelson, R.L.Robinson, W.T.Milner, J.L.C.Ford, Jr.

Coulomb Excitation of States in the Chromium Nuclei

NUCLEAR REACTIONS 50,52,53,54Cr(16O, 16O'γ), E=33 MeV; measured σ(Eγ, θ). 50,52,53,54Cr deduced levels, J, π, B(E2), B(M1). Enriched targets.


1966RO04      Phys.Rev. 146, 816 (1966)

R.L.Robinson, J.L.C.Ford, Jr., P.H.Stelson, G.R.Satchler

Elastic and Inelastic Proton Scattering from 106Pd and 108Pd

NUCLEAR STRUCTURE 106Pd, 108Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.146.816
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1965FO04      Bull.Am.Phys.Soc. 10, No.1, 105, JD14 (1965)

J.L.C.Ford, Jr., R.L.Robinson, P.H.Stelson

Elastic and Inelastic Scattering of Protons from 106Pd and 108Pd

NUCLEAR STRUCTURE 106Pd, 108Pd; measured not abstracted; deduced nuclear properties.


1965FO05      Nucl.Phys. 63, 588 (1965)

J.L.C.Ford, Jr., J.K.Bair, C.M.Jones, H.B.Willard

The 18O(α, p) Reaction and the Beta Decay of 21F

NUCLEAR REACTIONS 18O(d, p), E=7.76-9.95 MeV; measured σ(E). 22Ne deduced levels. Enriched target. 21F; measured T1/2.

doi: 10.1016/0029-5582(65)90745-5
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1965MC05      Nucl.Phys. 66, 97 (1965)

F.K.McGowan, R.L.Robinson, P.H.Stelson, J.L.C.Ford, Jr.

Coulomb Excitation of Vibrational Triplet States and Octupole States in the Even Cadmium Nuclei

NUCLEAR REACTIONS 110,112,114,116Cd(16O, 16O'γ), E = 42-49 MeV, measured Iγ, Eγ, .γγ-coin; deduced B (λ). Enriched targets. 110,112,114,116Cd deduced B(λ). Enriched targets.

doi: 10.1016/0029-5582(65)90135-5
Citations: PlumX Metrics


1965RO09      Nucl.Phys. 74, 281 (1965)

R.L.Robinson, P.H.Stelson, F.K.McGowan, J.L.C.Ford, Jr., W.T.Milner

Gamma Ray Energies Determined with a Lithium-Drifted Germanium Detector

NUCLEAR REACTIONS 48Ti, 50Cr, 56Fe, 64,66,68,70Zn, 70,72,74,76Ge, 75As, 76,78,80,82Se(α, α'γ), 79Br, 94,96,98,100Mo, 96,100,104Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 116,117,118,120,122,124Sn, 121,123Sb, 122,124,126,128,130Te, 195Pt(α, α'γ), E=6-9 MeV; measured Eγ. 77Se, 119Sn(α, α'γ), E=6-9 MeV; measured Eγ, Iγ. 18O(α, nγ), E=6-9 MeV; measured Eγ. 21Ne deduced level. Enriched targets.

RADIOACTIVITY 7Be, 22Na, 51Cr, 54Mn, 60Co, 65Zn, 88Y, 137Cs, 198Au, 203Hg, 207Bi; measured Eγ. 102,106Rh; measured Eγ, Iγ.

doi: 10.1016/0029-5582(65)90082-9
Citations: PlumX Metrics


1965RO11      ORNL-3778, p.112 (1965)

R.L.Robinson, F.K.McGowan, J.L.C.Ford, Jr.

Low-Lying Levels in 75As


1964FO05      Nucl.Phys. 55, 43 (1964)

J.L.C.Ford, Jr., J.K.Bair, R.L.Robinson, H.B.Willard

A Search for Interference Effects between Nuclear Resonance and Coulomb Excitation in the Na23(p, p') Reaction

NUCLEAR REACTIONS 23Na(p, p'γ), E ≈ 0.873 MeV; measured σ(E).

doi: 10.1016/0029-5582(64)90126-9
Citations: PlumX Metrics


1964FO13      Phys.Rev. 136, B953 (1964)

J.L.C.Ford, Jr.

Elastic scattering of deuterons by lithium-7

NUCLEAR REACTIONS 7Li(d, d), E=393 keV-1.7 MeV; measured products, 7Li; deduced σ(θ). Data were imported from EXFOR entry A1429.

doi: 10.1103/PhysRev.136.B953
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1429.


1964MC03      Bull.Am.Phys.Soc.9, No.1, 107, KC5 (1964)

F.K.McGowan, R.L.Robinson, P.H.Stelson, J.L.C.Ford, W.T.Milner

Coulomb Excitation of Vibrational Triplet States and Octupole States in Even Cadmium Nuclei

NUCLEAR STRUCTURE 114Cd, 116Cd, 112Cd, 110Cd; measured not abstracted; deduced nuclear properties.


1964MC18      ORNL-3582, p.107 (1964)

F.K.McGowan, P.H.Stelson, R.L.Robinson, J.L.C.Ford, W.T.Milner

Coulomb Excitation of Vibrational Triplet States and Octupole States in the Even Cadmium Nuclei

NUCLEAR STRUCTURE 114Cd, 116Cd, 112Cd, 110Cd; measured not abstracted; deduced nuclear properties.


1964PO02      Phys.Rev. 134, B1237 (1964)

D.Powers, J.K.Bair, J.L.C.Ford, Jr., H.B.Willard

Elastic Scattering of Alpha Particles by O18

NUCLEAR STRUCTURE 22Ne; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.134.B1237
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0750.


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