NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = P.H.Stelson Found 186 matches. Showing 1 to 100. [Next]1993BR11 Phys.Rev. C48, 1147 (1993) M.E.Brandan, J.R.Alfaro, A.Menchaca-Rocha, J.Gomez del Campo, G.R.Satchler, P.H.Stelson, H.J.Kim, D.Shapira Elastic Scattering of 58Ni + 27Al at Near-Barrier Energies NUCLEAR REACTIONS 27Al(58Ni, 58Ni), E=155-220 MeV; measured σ(E, θ); deduced optical model parameters, potential volume integrals. Phenomenological folding model, dispersion relations analyses.
doi: 10.1103/PhysRevC.48.1147
1993SH06 Phys.Rev. C47, 1666 (1993) Role of Neutron Flow in the Enhancement of Heavy Ion Fusion at Energies Below the Coulomb Barrier and the Systematics of Threshold Barriers NUCLEAR REACTIONS 89,90Zr(51Ti, X), E(cm) ≈ 98-120 MeV; calculated sub-barrier fusion σ(E); deduced neutron flow features. Many other target + projectile systems included.
doi: 10.1103/PhysRevC.47.1666
1991KI01 Phys.Rev. C43, 1231 (1991) H.J.Kim, J.Gomez del Campo, D.Shapira, P.H.Stelson, D.Napoli Multinucleon-Transfer Reactions for the 50Ti + 93Nb System at Sub- and Near-Barrier Energies NUCLEAR REACTIONS 50Ti(93Nb, X), E=283.1-306.9 MeV; measured fragment energy, charge spectra, σ(fragment θ); deduced multi-nucleon transfer probabilities.
doi: 10.1103/PhysRevC.43.1231
1991RO01 Phys.Lett. 254B, 25 (1991) N.Rowley, G.R.Satchler, P.H.Stelson On the ' Distribution of Barriers ' Interpretation of Heavy-Ion Fusion NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-65 MeV; analyzed data; deduced potential barriers distribution features.
doi: 10.1016/0370-2693(91)90389-8
1990ST04 Phys.Rev. C41, 1584 (1990) P.H.Stelson, H.J.Kim, M.Beckerman, D.Shapira, R.L.Robinson Fusion Cross Sections for 46,50Ti + 90Zr, 93Nb and Some Systematics of Heavy-Ion Fusion at Barrier and Subbarrier Energies NUCLEAR REACTIONS, ICPND 90Zr, 93Nb(46Ti, X), (50Ti, X), E(cm)=100.29-117.6 MeV; measured σ(fragment θ). 58,64Ni(32S, X), (28Si, X), E(cm)=56-62 MeV; 93Nb, 100Mo(32S, X), (36S, X), E(cm)=71-91 MeV; 184W(16O, X), E(cm) ≈ 60-100 MeV; calculated fusion σ(E).
doi: 10.1103/PhysRevC.41.1584
1988AH01 Phys.Rev. C37, 1836 (1988) A.Ahmad, G.Bomar, H.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, R.M.Ronningen, O.Scholten, P.H.Stelson Coulomb Excitation of 144, 146, 148, 150Nd NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E=10.5, 11 MeV; measured σ(Eα) following Coulomb excitation. 144,146,148,150Nd deduced B(E2), B(E3), hexadecapole transition matrix element. Enriched targets.
doi: 10.1103/PhysRevC.37.1836
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
1988HA26 Phys.Rev. C38, 572 (1988) B.A.Harmon, D.Shapira, P.H.Stelson, B.L.Burks, K.A.Erb, B.Shivakumar, K.Teh, S.T.Thornton Effect of Entrance Channel Asymmetry of Fusion Reactions Leading to Compound Nuclei with A = 40, 42 NUCLEAR REACTIONS 12C(28Si, X), E=6.4, 7.8, 9.4 MeV/nucleon; 12C(30Si, X), E=5.2, 5.7, 6.4, 7.5, 8.3 MeV/nucleon; measured fusion σ; deduced entrance channel asymmetry role.
doi: 10.1103/PhysRevC.38.572
1988KI09 Phys.Rev. C38, 2081 (1988) H.J.Kim, J.Gomez del Campo, M.M.Hindi, D.Shapira, P.H.Stelson Transfer Reactions for the 50Ti + 90Zr System below the Coulomb Barrier NUCLEAR REACTIONS 50Ti(90Zr, X), E=274-303 MeV; measured quasielastic σ(θ); deduced (90Zr, 49Ti), (90Zr, 51V) reaction probabilities.
doi: 10.1103/PhysRevC.38.2081
1988SH03 Phys.Rev. C37, 652 (1988) B.Shivakumar, D.Shapira, P.H.Stelson, S.Ayik, B.A.Harmon, K.Teh, D.A.Bromley 28Si + 14N Orbiting Interaction NUCLEAR REACTIONS 14N(28Si, 14N), E=100 MeV; 14N(28Si, 16O), E=140 MeV; 14N(28Si, 12C), E=100-170 MeV; measured ejectile yields. 28Si(14N, X), E=100-170 MeV; measured orbiting σ(E) for X=10,11B, 11,12,13C, 13,14,15N, 15,16,17O, 17,18,19F, 19,20,21Ne; deduced critical angular momentum.
doi: 10.1103/PhysRevC.37.652
1988SI01 Phys.Rev. C37, 158 (1988) J.D.Silk, H.D.Holmgren, D.L.Hendrie, T.J.M.Symons, G.D.Westfall, P.H.Stelson, S.Raman, R.L.Auble, J.R.Wu, K.Van Bibber Fragmentation of 16O Projectiles at 100 MeV per Nucleon NUCLEAR REACTIONS 27Al(16O, 12CX), E=100 MeV/nucleon; measured invariant σ vs rapidity. 27Al(16O, X), E=100 MeV/nucleon; measured σ(fragment θ), σ vs fragment mass for X=7,9,10Be, 10,11,12B, 10,11,12,13,14C, 13,14,15N; deduced reaction mechanism.
doi: 10.1103/PhysRevC.37.158
1988ST08 Phys.Lett. 205B, 190 (1988) Neutron Flow between Nuclei as the Principal Enhancement Mechanism in Heavy-Ion Subbarier Fusion NUCLEAR REACTIONS 58Ni(58Ni, X), E ≈ 93-110 MeV; 64Ni(64Ni, X), E(cm) ≈ 90-110 MeV; calculated fusion σ(E); deduced barrier distribution, neutron flow role.
doi: 10.1016/0370-2693(88)91647-4
1987GO01 Phys.Rev. C35, 137 (1987) J.Gomez del Campo, D.E.DiGregorio, J.A.Biggerstaff, Y.D.Chan, D.C.Hensley, P.H.Stelson, D.Shapira, M.E.Ortiz Correlations between α Particles and Evaporation Residues for the 14N + 12C Reaction at E(14N) = 180 MeV NUCLEAR REACTIONS 12C(14N, xα), E=180 MeV; measured α(evaporation residues)(θ); deduced equilibrium, nonequilibrium effects. ΔE-E solid state detectors.
doi: 10.1103/PhysRevC.35.137
1987RA01 At.Data Nucl.Data Tables 36, 1 (1987) S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson Transition Probability, B(E2), from the Ground to the First-Excited 2+ State of Even-Even Nuclides COMPILATION A=6-254; compiled, evaluated 2+ level energies, B(E2), T1/2, β2, β2/β2(sp), EWSR, intrinsic quadrupole moments.
doi: 10.1016/0092-640X(87)90016-7
1986SC30 Phys.Rev. C34, 1962 (1986) O.Scholten, R.M.Ronningen, A.Y.Ahmed, G.O.Bomar, H.L.Crowell, J.H.Hamilton, H.Kawakami, C.F.Maguire, W.G.Nettles, R.B.Piercey, A.V.Ramayya, R.Soundranayagam, P.H.Stelson Mass Dependence of Effective Charges in the Interacting-Boson Model NUCLEAR REACTIONS 144,146,148,150Nd(α, α'), E not given; measured Coulomb excitation. 144,146,148,150Nd levels deduced B(E2). Magnetic spectrometer. Interacting boson model. NUCLEAR STRUCTURE 142,144,146,148,150Nd; calculated B(E2), effective charges. Interacting boson model.
doi: 10.1103/PhysRevC.34.1962
1986SH25 Phys.Rev.Lett. 57, 1211 (1986) B.Shivakumar, D.Shapira, P.H.Stelson, M.Beckerman, B.A.Harmon, K.Teh, D.A.Bromley Equilibration in Orbiting Reactions NUCLEAR REACTIONS 14N(28Si, 14N), E=100-170 MeV; measured ejectile yield at θ=15°, absolute orbiting σ(E). 14N(28Si, 12C), (28Si, 16O), E=100-170 MeV; measured absolute orbiting σ(E); deduced charge, mass equilibration.
doi: 10.1103/PhysRevLett.57.1211
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
1984GO05 Phys.Rev. C29, 1722 (1984) J.Gomez del Campo, J.A.Biggerstaff, R.A.Dayras, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad Comparison of Fusion Cross Sections for the 10B + 16O and 12C + 14N Systems NUCLEAR REACTIONS, ICPND 12C(14N, X), E=158, 248 MeV; 10B(16O, X), E=203.6 MeV; measured σ(fragment θ, E) for fragment Z=3, 10, fusion, reaction, direct σ(E), fragment velocity spectra. 16O(10B, X), E=42-169.7 MeV; measured fusion, reaction σ(E). 10B(16O, X), E=203.6 MeV; measured evaporation residue σ(θ). 12C(14N, X), E=182 MeV; measured evaporation residue relative yield. Monte Carlo Hauser-Feshbach calculations.
doi: 10.1103/PhysRevC.29.1722
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
1983RA21 Phys.Rev. C28, 602 (1983); Erratum Phys.Rev. C29, 344 (1984) S.Raman, B.Fogelberg, J.A.Harvey, R.L.Macklin, P.H.Stelson, A.Schroder, K.-L.Kratz Overlapping β Decay and Resonance Neutron Spectroscopy of Levels in 87Kr NUCLEAR REACTIONS 86Kr(n, n), (n, X), E=1-400 keV; measured σ(E), transmission. 86Kr(n, γ), E=1-90 keV; measured σ(capture) vs E. 87Kr deduced resonances, L, J, π, Γγ, (gΓγ), (gΓn), (gΓnΓγ/Γ), neutron strength function, Maxwellian < σ >. Enriched target. Multi-level R-matrix analysis. RADIOACTIVITY 87Br(β-), (β-n) [from 235U(n, F)]; measured Eγ, Iγ, γγ-coin, β-delayed En; deduced J, π, log ft, Gamow-Teller matrix elements. 87Kr deduced levels, β-branching, J, π.
doi: 10.1103/PhysRevC.28.602
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
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
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
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
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
1979FU04 Phys.Rev. C20, 670 (1979) C.B.Fulmer, R.M.Wieland, D.C.Hensley, S.Raman, G.R.Satchler, A.H.Snell, P.H.Stelson, R.G.Stokstad 12C + 12C Transfer Reactions at 93.8 MeV NUCLEAR REACTIONS 12C(12C, 11C), (12C, 11B), (12C, 10B), E=93.8 MeV; measured σ(θ). 13C, 13N levels deduced S. DWBA analysis.
doi: 10.1103/PhysRevC.20.670
1979GO09 Phys.Rev.Lett. 43, 26 (1979) J.Gomez del Campo, R.A.Dayras, J.A.Biggerstaff, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad Comparison of Fusion Cross Sections for 10B + 16O → 26Al and 12C + 14N → 26Al NUCLEAR REACTIONS 10B(16O, X), E(cm)=15-80 MeV; measured σ(fusion, E), σ(direct, E).
doi: 10.1103/PhysRevLett.43.26
1979GO11 Phys.Rev. C19, 2170 (1979) J.Gomez del Campo, R.G.Stokstad, J.A.Biggerstaff, R.A.Dayras, A.H.Snell, P.H.Stelson Fusion and Peripheral Reactions of 12C + 14N at Energies up to 13 MeV/A NUCLEAR REACTIONS 12C(14N, X), E=34.1-178.1 MeV; measured σ(θ) of evaporation residues; deduced fusion, direct, total σ. Hauser-Feshbach, optical model calculations.
doi: 10.1103/PhysRevC.19.2170
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
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
1979ST10 Phys.Rev. C20, 655 (1979) R.G.Stokstad, R.M.Wieland, G.R.Satchler, C.B.Fulmer, D.C.Hensley, S.Raman, L.D.Rickertsen, A.H.Snell, P.H.Stelson Elastic and Inelastic Scattering of 12C by 12C from E = 35-63 MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E(cm)=35-63 MeV; measured σ(E, θ). Optical model, DWBA, coupled-channels analysis.
doi: 10.1103/PhysRevC.20.655
1978MC02 Nucl.Phys. A297, 51 (1978) F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson, Z.W.Grabowski Coulomb Excitation of Vibrational-Like States in 166-170Er NUCLEAR REACTIONS 166,168,170Er(α, α'γ), E=14 MeV; measured Iγ, Eγ, γ(θ). 166,168,170Er levels deduced B(E2), B(M1), B(E3), J, π, δ. Enriched targets.
doi: 10.1016/0375-9474(78)90198-7
1977DA12 Nucl.Phys. A284, 484 (1977) W.K.Dagenhart, P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, S.Raman, W.K.Tuttle III Coulomb Excitation of 115Sn NUCLEAR REACTIONS 115Sn(α, α'γ), (α, α'), E=7.0-10.6 MeV; 115Sn(16O, 16O'γ), E=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening, Eα'. 115Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.
doi: 10.1016/0375-9474(77)90398-0
1977MA13 Nucl.Data Sheets 21, 1 (1977) Nuclear Data Sheets for A = 184 COMPILATION 184Hf, 184Ta, 184W, 184Re, 184Os, 184Ir, 184Pt, 184Au, 184Hg, 184Tl; compiled, evaluated structure data.
doi: 10.1016/S0090-3752(77)80091-4
1977MC11 Nucl.Phys. A289, 253 (1977) F.K.McGowan, W.T.Milner, R.O.Sayer, R.L.Robinson, P.H.Stelson Coulomb Excitation of 182,184,186W and 166Er with 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(α, α'γ), E=15 MeV; 186W(16O, 16O'γ), E=42 MeV; 166Er(α, α'γ), E=13.5 MeV; 166Er(16O, 16O'γ), E=42 MeV; measured Iγ, Eγ, γ(θ), αγ-coin, 16Oγ-coin. 182W levels deduced J. 184W levels deduced B(EL), J. 186W levels deduced B(EL), J, quadrupole moment. 166Er deduced quadrupole moment. Enriched, natural targets.
doi: 10.1016/0375-9474(77)90532-2
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
1977RO16 Phys.Rev. C16, 571 (1977) R.M.Ronningen, R.B.Piercey, A.V.Ramayya, J.H.Hamilton, S.Raman, P.H.Stelson, W.K.Dagenhart Coulomb Excitation of 2+ and 3- States in 192Pt and 194Pt NUCLEAR REACTIONS 192,194Pt(α, α'), E=14.9 MeV; measured Coulomb excitation. 192,194Pt levels deduced B(E2), B(E3). Enriched targets.
doi: 10.1103/PhysRevC.16.571
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
1977ST25 Phys.Lett. 70B, 289 (1977) R.G.Stokstad, R.A.Dayras, J.Gomez del Campo, P.H.Stelson, C.Olmer, M.S.Zisman Measurements of the Fusion of 12C + 14N and the Liquid-Drop Limit for 26Al NUCLEAR REACTIONS 12C(14N, X), E=248 MeV; measured fusion σ.
doi: 10.1016/0370-2693(77)90660-8
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
1976GU10 Nucl.Phys. A262, 96 (1976) D.E.Gustafson, J.Gomez del Campo, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair High-Spin States of 26Mg Populated in the 12C(18O, α) Reaction NUCLEAR REACTIONS 12C(18O, α), E=43.2-45.9 MeV; measured σ(E) at θlab=7°. 26Mg deduced levels, K, J, π. Hauser-Feshbach calculations, suggested J, π values.
doi: 10.1016/0375-9474(76)90442-5
1976RO15 Phys.Rev. C14, 2126 (1976) R.L.Robinson, J.K.Bair, C.H.Johnson, P.H.Stelson, W.B.Dress, C.M.Jones Cross Sections for the Ni, Cu, Zn(16,18O, xn) Reactions Near the Coulomb Barrier NUCLEAR REACTIONS 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(16O, xn), (18O, xn), E=36-55 MeV; measured total σ(E).
doi: 10.1103/PhysRevC.14.2126
1976ST07 Phys.Rev.Lett. 36, 1529 (1976) R.G.Stokstad, J.Gomez del Campo, J.A.Biggerstaff, A.H.Snell, P.H.Stelson Fusion of 14N + 12C at Energies up to 178 MeV NUCLEAR REACTIONS 12C(14N, X), E=43-178 MeV; measured fusion σ(E).
doi: 10.1103/PhysRevLett.36.1529
1976TU02 Phys.Rev. C13, 1036 (1976) W.K.Tuttle III, P.H.Stelson, R.L.Robinson, W.T.Milner, F.K.McGowan, S.Raman, W.K.Dagenhart Coulomb Excitation of 113,115In NUCLEAR REACTIONS 113,115In(α, α'γ), E=9.4, 10, 10.6 MeV; 113,115In(16O, 16O'γ), E=42, 45 MeV; measured Coulomb excitation, DSA, Eγ, Iγ, γ(θ). 113,115In deduced levels, J, π, T1/2, B(E2), B(M1).
doi: 10.1103/PhysRevC.13.1036
1975GO25 Phys.Rev. C12, 1247 (1975) J.Gomez del Campo, D.E.Gustafson, R.L.Robinson, P.H.Stelson, P.D.Miller, J.K.Bair, J.B.McGrory Population of High-Spin States in 23Na Through the 11B(16O, α) Reaction NUCLEAR REACTIONS 11B(16O, α), E=41.6-45.4 MeV; measured σ(E, Eα, θ). 23Na deduced levels, J, π.
doi: 10.1103/PhysRevC.12.1247
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
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
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
1974HA44 Phys.Lett. 51B, 341 (1974) M.L.Halbert, C.B.Fulmer, S.Raman, M.J.Saltmarsh, A.H.Snell, P.H.Stelson Elastic Scattering of 16O by 16O NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=35-88 MeV; measured σ(E, θ).
doi: 10.1016/0370-2693(74)90223-8
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
1974RI12 Phys.Rev.Lett. 33, 1346 (1974) L.L.Riedinger, G.J.Smith, P.H.Stelson, E.Eichler, G.B.Hagemann, D.C.Hensley, N.R.Johnson, R.L.Robinson, R.O.Sayer Dominance of the i13/2 Neutron in Yb Backbending NUCLEAR REACTIONS 148Nd(22Ne, 5nγ), E=109 MeV; measured Eγ, γγ-coin. 156Gd(12C, 3nγ), E=58 MeV; measured Eγ, γ(θ). 165Yb deduced levels, J, π, decoupled rotational bands.
doi: 10.1103/PhysRevLett.33.1346
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
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
1973RA17 Nucl.Phys. A206, 343 (1973) S.Raman, P.H.Stelson, G.G.Slaughter, J.A.Harvey, T.A.Walkiewicz, G.J.Lutz, L.G.Multhauf, K.G.Tirsell Gamma Transitions between Low-Lying Levels in 119Sn RADIOACTIVITY 119In [from 120Sn(γ, p), 119Sn(n, p), 122Sn(n, α) (β) 119In]; measured T1/2, Eγ, Iγ. 119Sn deduced levels. NUCLEAR REACTIONS 118Sn(n, γ), En=th, 46-5000 eV; measured Eγ, Iγ. 119Sn(α, α'γ), Eα=10 MeV; measured Eγ, Iγ. 119Sn deduced levels. Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(73)90538-1
1973ST10 Priv.Comm. (June 1973); See Also 73Ri04, 73St09
1973ST14 Phys.Rev. C8, 368 (1973) P.H.Stelson, S.Raman, J.A.McNabb, R.W.Lide, C.R.Bingham Search for a Zero-Phonon Gamma-Ray Transition in 108Pd and 134Ba RADIOACTIVITY 108mAg, 134Cs; measured Iγ. 108Pd, 134Ba deduced upper limit on intensity of zero phonon γ-transition.
doi: 10.1103/PhysRevC.8.368
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
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
1972RO27 Nucl.Phys. A193, 14 (1972) R.L.Robinson, F.K.McGowan, W.T.Milner, P.H.Stelson Coulomb Excitation of 81Br NUCLEAR REACTIONS 81Br(α, α'γ), E=2.5-8.2 MeV; 81Br(16O, 16O'γ), E=33 MeV; measured σ(E;Eγ, θ(γ), θ(γγ)), Iγ, Doppler broadening. 81Br deduced levels, J, π, B(E2), B(M1), T1/2.
doi: 10.1016/0375-9474(72)90231-X
1972ST16 Nucl.Phys. A190, 197 (1972) P.H.Stelson, W.T.Milner, F.K.McGowan, R.L.Robinson, S.Raman Coulomb Excitation of 117,119Sn NUCLEAR REACTIONS 117,119Sn(α, α'γ), 117,119Sn(16O, 16O'γ)Eα=10, 10.5, 11 MeV;E(16O)=45 MeV; measured Eγ, Iγ, Iγ(θ), Doppler broadening. 117,119Sn deduced levels, J, π, B(E2), B(M1), T1/2. Enriched targets.
doi: 10.1016/0375-9474(72)90137-6
1972ST23 Priv.Comm. (August 1972)
1972ST39 Nucl.Instrum.Methods 98, 481 (1972) P.H.Stelson, J.K.Dickens, S.Raman, R.C.Trammell Deterioration of Large Ge(Li) Diodes Caused by Fast Neutrons
doi: 10.1016/0029-554X(72)90232-7
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
1971HA17 Nucl.Phys. A172, 139 (1971) J.H.Hamilton, S.M.Brahmavar, J.B.Gupta, R.W.Lide, P.H.Stelson Search for Weak Transitions in the Decay of 108mAg RADIOACTIVITY 108mAg [from 107Ag(n, γ)]; measured Eγ, Iγ; deduced isomeric branching. Ge(Li) detectors. Sources produced 1950'S, 1960'S.
doi: 10.1016/0375-9474(71)90121-7
1971MC14 Ann.Phys.(N.Y.) 63, 549 (1971) F.K.McGowan, W.T.Milner, R.L.Robinson, P.H.Stelson Coulomb Excitation of 197Au and a Core-Excitation Analysis NUCLEAR REACTIONS 197Au(α, α'γ), E=9.94-14 MeV; 197Au(16O, 16O'γ), E=42-45 MeV; measured σ(E;Eγ, θ(γ)), γγ-coin. 197Au levels deduced B(E2), B(M1), γ-mixing, g. Coulomb excitation;core-excitation analysis.
doi: 10.1016/0003-4916(71)90028-5
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
1971MI08 Nucl.Phys. A177, 1 (1971) W.T.Milner, F.K.McGowan, R.L.Robinson, P.H.Stelson, R.O.Sayer Coulomb Excitation of 182,184,186W, 186,188,190,192Os and 192,194,196,198Pt with Protons, 4He and 16O Ions NUCLEAR REACTIONS 182,184,186W(p, p'γ), E=5 MeV;182,184,186W(α, α'γ), E=14, 15 MeV; 182,184,186W(16O, 16O'γ), E=45.5 MeV; 188,190,192Os(p, p'γ), E=4.56-5.08 MeV; 186Os(α, α'γ), E=3-5 MeV; 188,190,192Os(α, α'γ), E=15 MeV; 186,188,190,192Os(16O, 16O'γ), E=42, 45.1, 45.5 MeV; 192,194,196,198Pt(p, p'γ), E=4.5 MeV; 192,194,196,198Pt(16O, 16O'γ), E=43.75 MeV; measured Iγ, Eγ, (16O)(γ)-coin, 182,184,186W, 186,188,190,192Os, 192,196,194,198Pt deduced B(E2), B(M1), J. Enriched, natural targets.
doi: 10.1016/0375-9474(71)90161-8
1971RO09 Nucl.Phys. A166, 141 (1971) R.L.Robinson, W.T.Milner, F.K.McGowan, P.H.Stelson, M.A.Ludington E2/M1 Admixture of the 2'→2 Transition in 108Pd NUCLEAR REACTIONS 108Pd(α, α'γγ), Eα=10.1 MeV; measured γγ(θ). 108Pd transition deduced γ-mixing, B(E2), B(M1). Enriched target.
doi: 10.1016/0375-9474(71)90418-0
1971ST15 Priv.Comm. (July 1971)
1970BA64 Phys.Rev. C2, 2154 (1970) Levels of 61Cu, 64Cu, 67Ga, and 68Ga Excited by the (p, n) Reaction NUCLEAR REACTIONS 61,64Ni, 67,68Zn(p, n), E=2.9-6.3 MeV; measured σ(E;En). 61Cu deduced levels. 64Cu, 67,68Ga deduced levels, J, π.
doi: 10.1103/PhysRevC.2.2154
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
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
1970RO14 Nucl.Phys. A150, 225 (1970) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Coulomb Excitation of 107,109Ag NUCLEAR REACTIONS 107,109Ag(α, α'γ), E=10.0, 10.7 MeV; 107,109Ag(16O, 16O'γ), E=45.5 MeV; measured σ(Eγ, θ(γ)), γγ-triple correlation, Doppler broadening. 107,109Ag deduced levels, B(E2), B(M1), B(E1), T1/2, J, π, γ-mixing, γ-branching.
doi: 10.1016/0375-9474(70)90946-2
1970SA09 Phys.Rev. C1, 1525 (1970) R.O.Sayer, P.H.Stelson, F.K.McGowan, W.T.Milner, R.L.Robinson Multiple Coulomb Excitation of 152Sm, 166Er, and 172,174,176Yb NUCLEAR REACTIONS 152Sm, 166Er, 172,174,176Yb(α, α'γ), E=7, 8, 9, 10 MeV; 152Sm, 166Er, 172,174,176Yb(16O, 16O'γ), E=25-52 MeV; measured σ(E;Eα', Eγ), σ(E;E(16O'), Eγ). 152Sm, 166Er, 172,174,176Yb levels deduced B(E2).
doi: 10.1103/PhysRevC.1.1525
1970ST05 Nucl.Phys. A144, 254 (1970) P.H.Stelson, R.W.Lide, C.R.Bingham Decay of the γ-Vibrational Band in 250Cf RADIOACTIVITY 250Bk[from 254Es source]; measured Eγ, Iγ. 250Cf deduced levels, B(E2) ratios, γ-mixing. Ge(Li) detector.
doi: 10.1016/0375-9474(70)90358-1
1970ST20 Phys.Rev. C2, 2015 (1970) P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner Static Quadrupole Moment of the First 2+ States of the Even Tin Nuclei NUCLEAR REACTIONS 112,116,118,120,122,124Sn(α, α'γ), E=10 MeV; 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=46 MeV; measured σ(Eα', Eγ), σ(E(16O'), Eγ). 112,116,118,120,122,124Sn levels deduced quadrupole moment, B(E2).
doi: 10.1103/PhysRevC.2.2015
1970TA01 Phys.Rev. C2, 160 (1970) S.Tanaka, P.H.Stelson, W.T.Bass, J.Lin Levels in 53Mn, 58Co, 63Zn, and 70Ga from the (p, n) Reaction NUCLEAR REACTIONS 53Cr, 58Fe, 63Cu, 70Zn(p, n), E=2.74-6.35 MeV; measured σ(E;En). 53Mn, 58Co, 63Zn, 70Ga deduced levels.
doi: 10.1103/PhysRevC.2.160
1969MI07 Nucl.Phys. A129, 687 (1969) W.T.Milner, F.K.McGowan, P.H.Stelson, R.L.Robinson, R.O.Sayer Coulomb Excitation of the Even-A Cadmium Nuclei NUCLEAR REACTIONS 106,108,110,112,114,116Cd(p, p'γ), E=2.7, 3.0 MeV; 106,108,110,112,114,116Cd(α, α'γ), E=9-11 MeV; 106,108Cd(16O, 16O'γ), E=42-49 MeV; measured Iγ, Eγ, γγ-coin, γ(θ). 106,108,110,112,114,116Cd deduced levels, B(E2), B(M1), J. Enriched targets.
doi: 10.1016/0375-9474(69)90710-6
1969RO03 Nucl.Phys. A123, 193 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Gamma-Gamma Angular Correlations Following Coulomb Excitation NUCLEAR REACTIONS 107,109Ag, 110Pd, 117Sn(α, α'γ), E=9.5-10 MeV; 190,192Os(p, p'γ), E=4.5 MeV; measured γγ(θ). 107,109Ag, 110Pd, 117Sn, 190,192Os deduced levels, J, γ-mixing ratio. Enriched target.
doi: 10.1016/0375-9474(69)90899-9
1969RO05 Nucl.Phys. A124, 553 (1969) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner, R.O.Sayer Coulomb Excitation of 106,108,110Pd NUCLEAR REACTIONS 106,108,110Pd(α, α'γ), E=9-10 MeV; 106,108,110Pd(16O, 16O'γ), E=42-49 MeV, measured Iγ, Eγ, γγ-coin., γ(θ). 106,108,110Pd deduced levels B(E2), B(M1), T1/2, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90650-2
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
1968EI02 Nucl.Phys. A120, 622 (1968) E.Eichler, P.H.Stelson, J.K.Dickens A New Measurement of the Half-Life of the 72Ge 0+ State NUCLEAR REACTIONS 19F, 72Ge(n, n') E=4.75 MeV; measured nX-delay. 19F, 72Ge level deduced T1/2. Natural target.
doi: 10.1016/0375-9474(68)90468-5
1968MC08 Nucl.Phys. A113, 529 (1968) F.K.McGowan, R.L.Robinson, P.H.Stelson, W.T.Milner Coulomb Excitation of States in the Even-Mass Ruthenium Nuclei with 16O and 4He Ions NUCLEAR REACTIONS 98,100,102,104Ru(16O, 16O'γ), E=42-49 MeV; 98,100,102,104Ru(α, α'γ), E=10 MeV; measured σ(Eγ, θ), γγ-coin; deduced B(E2), B(M1), J. Enriched targets.
doi: 10.1016/0375-9474(68)90161-9
1968ST05 Nucl.Phys. A111, 331 (1968) Decay of 65Zn RADIOACTIVITY 65Zn; measured Iγ, γγ-coin. 65Cu level deduced branching. Ge(Li) detector.
doi: 10.1016/0375-9474(68)90126-7
1968ST07 Priv.Comm. (1968) NUCLEAR STRUCTURE 65Cu; measured not abstracted; deduced nuclear properties.
1968ST14 Phys.Rev. 170, 1172 (1968) P.H.Stelson, F.K.McGowan, R.L.Robinson, W.T.Milner, R.O.Sayer Coulomb Excitation of the Even Tin Nuclei NUCLEAR STRUCTURE 112Sn, 118Sn, 116Sn, 120Sn, 122Sn, 124Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.1172
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
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
1967MA18 Priv.Comm. (1967) NUCLEAR STRUCTURE 59Cu; measured not abstracted; deduced nuclear properties.
1967RO03 Nucl.Phys. A96, 6 (1967) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Low-Lying Levels of 79Br RADIOACTIVITY 79Kr [from 79Br(p, n), 78Kr(n, γ)]; measured Eγ, Iγ, γγ coin. 79Br deduced levels, B(E2), B(M1), T1/2, J, π, log ft. 79Br(α, α'γ), E = 2.5-7 MeV; 79Br(16O, 16O'γ), E = 36 MeV; measured Eγ, Iγ, γγ coin, γ(θ). Enriched target.
doi: 10.1016/0375-9474(67)90690-2
1967RO14 Nucl.Phys. A104, 401 (1967) R.L.Robinson, F.K.McGowan, P.H.Stelson, W.T.Milner Coulomb Excitation of 75As NUCLEAR REACTIONS 75As(α, α'γ), E=3.5-8.1 MeV; 75As(16O, 16O'γ), E=36-38 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 75As deduced levels, B(E2), B(M1), T1/2, J, π.
doi: 10.1016/0375-9474(67)90564-7
1967ST05 Phys.Rev. 157, 1098 (1967) Decay of 124Sb to 124Te NUCLEAR STRUCTURE 124Sb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.157.1098
1967ST11 Priv.Comm. (1967) NUCLEAR STRUCTURE 59Co; measured not abstracted; deduced nuclear properties.
1967ST15 Priv.Comm. (1967) NUCLEAR STRUCTURE 65Zn; measured not abstracted; deduced nuclear properties.
1967ST18 Priv.Comm. (1967) NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.
1967ST19 Priv.Comm. (1967) P.H.Stelson, J.K.Dickens, F.G.Perey NUCLEAR STRUCTURE 59Ni; measured not abstracted; deduced nuclear properties.
1966BI15 ORNL-TM-1665, p.3 (1966) J.A.Biggerstaff, Y.Cassagnou, W.E.Kinney, M.V.Harlow, Jr., J.M.McConnell, F.G.Perey, P.H.Stelson Neutron Inelastic Scattering Program NUCLEAR STRUCTURE 59Ni, 59Cu, 59Co, 51V, 28Si, 60Cu, 65Zn, 56Fe, 53Mn, 51Cr, 55Fe, 40Ca, 39K, 12C, 89Y, 27Al, 23Na; measured not abstracted; deduced nuclear properties.
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