NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.L.Ford Found 109 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1964FO13 Phys.Rev. 136, B953 (1964) 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
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
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