NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.G.Harvey Found 102 matches. Showing 1 to 100. [Next]2003HA09 Phys.Rev. C 67, 044609 (2003) Explanation of difference in one-neutron knockout cross sections between odd-odd and even-even projectiles with equal neutron and proton numbers NUCLEAR REACTIONS 1H(12C, X), (14N, X), (16O, X), (20Ne, X), (22Na, X), (24Mg, X), (26Al, X), (28Si, X), (30P, X), (32S, X), (34Cl, X), (40Ca, X), E ≈ 600 MeV/nucleon; analyzed one-neutron removal σ; deduced odd-even staggering mechanism.
doi: 10.1103/PhysRevC.67.044609
1996HA25 Phys.Rev. C54, R1520 (1996) Spatial Separation of Outer Neutrons in 11Li NUCLEAR REACTIONS 12C(11Li, 2n9Li), E=280 MeV/nucleon; calculated neutron momentum distributions in coincidence with 9Li; deduced 2n-separation role.
doi: 10.1103/PhysRevC.54.R1520
1994HA15 Phys.Rev. C49, R2890 (1994) Momentum Distribution of Projectile Fragments and Nuclear Shape NUCLEAR REACTIONS C(12C, X), E=1000 MeV/nucleon; C(11Li, X), E=790 MeV/nucleon; calculated 11C, 9Li fragment transverse momentum distribution.
doi: 10.1103/PhysRevC.49.R2890
1990HA15 Phys.Lett. 238B, 11 (1990) Neutron Density Distribution in 11Li NUCLEAR STRUCTURE 11Li; analyzed reaction data; deduced neutron radial density distribution.
doi: 10.1016/0370-2693(90)92091-V
1990HA42 Phys.Lett. 252B, 536 (1990) Formation of Projectile Fragments by Statistical Decay in High-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 1H(12C, X), (14N, X), (16O, X), (20Ne, X), (24Mg, X), (27Al, X), (28Si, X), (32S, X), (40Ar, X), (40Ca, X), (56Fe, X), (58Ni, X), E=high; calculated σ for few nucleon removal from projectile.
doi: 10.1016/0370-2693(90)90478-O
1989HA43 Phys.Rev. C39, 841 (1989) B.G.Harvey, H.J.Crawford, P.J.Lindstrom, A.J.Cole Statistical Decay of Fragments from C + 12C, 2.1 GeV/nucleon
doi: 10.1103/PhysRevC.39.841
1985WA22 Phys.Rev. C32, 894 (1985) S.Wald, S.B.Gazes, C.R.Albiston, Y.Chan, B.G.Harvey, M.J.Murphy, I.Tserruya, R.G.Stokstad, P.J.Countryman, K.Van Bibber, H.Homeyer Transfer and Breakup Processes in Reactions of 11- and 17-MeV/nucleon 20Ne + 197Au NUCLEAR REACTIONS 197Au(20Ne, X), E=220, 341 MeV; measured σ(fragment E, θ, Z) for X=Li, Be, B, C, N, O, F; deduced transfer, breakup, primary ejectile yields. Coincidence techniques.
doi: 10.1103/PhysRevC.32.894
1984RA10 Phys.Rev. C30, 158 (1984) W.D.M.Rae, A.J.Cole, B.G.Harvey, R.G.Stokstad Breakup of 16O and 20Ne at 9 MeV/Nucleon NUCLEAR REACTIONS 12,13C, 28Si(16O, 16O'), (16O, 20Ne), E=140 MeV; 12C(20Ne, 20Ne), E=175 MeV; measured relative E spectra, α(12C)-, α(16O)-coin; deduced ejectile sequential breakup role.
doi: 10.1103/PhysRevC.30.158
1983HA36 Phys.Lett. 130B, 373 (1983) Dynamics of Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 197Au(20Ne, X), E=338 MeV; calculated σ(fragment E) vs fragment mass for X=Li, Be, B, C, N, O, F. 181Ta(20Ne, X), E=200 MeV; calculated angular momentum transfer to target vs fragment Z. Exact kinematics treatment, projectile target overlapping region for nucleon transfer.
doi: 10.1016/0370-2693(83)91525-3
1983MU01 Phys.Lett. 120B, 75 (1983) M.J.Murphy, B.G.Harvey, D.L.Hendrie, W.W.Pang, K.van Bibber, R.Legrain Transfer and Breakup Reactions in 16O + CsI at 16.4 MeV/n NUCLEAR REACTIONS Cs, I(16O, X), E=16.4 MeV/nucleon; measured fragment charge, energy, multiplicity; deduced reaction mechanism.
doi: 10.1016/0370-2693(83)90626-3
1981CO22 Phys.Rev.Lett. 47, 1705 (1981) A.J.Cole, W.D.M.Rae, M.E.Brandan, A.Dacal, B.G.Harvey, R.Legrain, M.J.Murphy, R.G.Stokstad 12C + 12C Reaction Cross Section between 70 and 290 MeV Obtained from Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=120-290 MeV; measured σ(θ) vs momentum transfer; deduced σ(total), σ(reaction).
doi: 10.1103/PhysRevLett.47.1705
1981LE03 Phys.Rev. C23, 552 (1981) D.Lebrun, M.Buenerd, M.Bini, B.G.Harvey, R.Legrain, J.Mahoney, T.J.M.Symons, K.Van Bibber Inelastic Scattering of 9Be of 27 MeV/A to Giant Resonances NUCLEAR REACTIONS 208Pb(9Be, 9Be'), E=245 MeV; measured σ(θ). 208Pb deduced excitation of GQR. DWBA analysis.
doi: 10.1103/PhysRevC.23.552
1981RA20 Phys.Lett. 105B, 417 (1981) W.D.Rae, A.J.Cole, A.Dacal, R.Legrain, B.G.Harvey, J.Mahoney, M.J.Murphy, R.G.Stokstad, I.Tserruya Coherent and Incoherent Processes in Projectile Breakup NUCLEAR REACTIONS 12,13C, 28Si(16O, α12C), E=140 MeV; measured 12Cα-coin, total, relative energies of fragments; deduced coherent, incoherent projectile breakup.
doi: 10.1016/0370-2693(81)91195-3
1980RA12 Phys.Rev.Lett. 45, 884 (1980) W.D.Rae, R.G.Stokstad, B.G.Harvey, A.Dacal, R.Legrain, J.Mahoney, M.J.Murphy, T.J.M.Symons Molecular Resonances and the Production of Fast α Particles in the Reaction of 16O with 12,13C Nuclei NUCLEAR REACTIONS 12,13C(16O, α), E=140 MeV; measured α12C-coin; deduced no molecular resonance or final-state interaction between carbon ions. 16O levels deduced excitation, decay probabilities.
doi: 10.1103/PhysRevLett.45.884
1978PI09 Phys.Rev. C18, 180 (1978) S.C.Pieper, M.H.Macfarlane, D.H.Gloeckner, D.G.Kovar, F.D.Becchetti, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, F.Puhlhofer, W.von Oertzen, M.S.Zisman Energy Dependence of Elastic Scattering and One-Nucleon Transfer Reactions Induced by 16O on 208Pb. I NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-216.6 MeV; 208Pb(16O, 15N), (16O, 17O), E=104, 138.5, 216.6 MeV; measured σ(θ). Optical model, DWBA analysis.
doi: 10.1103/PhysRevC.18.180
1976BU16 Phys.Rev.Lett. 37, 1191 (1976) M.Buenerd, C.K.Gelbke, B.G.Harvey, D.L.Hendrie, J.Mahoney, A.Menchaca-Rocha, C.Olmer, D.K.Scott Similarity of Cross Sections for Peripheral Collisions at 20 MeV/A and 2.1 GeV/A NUCLEAR REACTIONS 208Pb(16O, X), E=315 MeV; measured σ(A, Z).
doi: 10.1103/PhysRevLett.37.1191
1976VO07 Z.Phys. A279, 357 (1976) W.von Oertzen, H.Homeyer, B.G.Harvey, D.Hendrie, D.Kovar Two Proton Transfer Reactions between Pairing Rotational States with 104 MeV 16O on 142Nd, 144Sm, 148Sm and 152Sm NUCLEAR REACTIONS 142Nd, 144,148,152Sm(16O, 14C), E=104 MeV; measured σ(E(14C), θ). 144Sm(16O, 12C), (16O, 13C), E=104 MeV; measured σ. 144Sm, 146,150,154Gd deduced levels.
1975BE11 Nucl.Phys. A242, 149 (1975) M.Bernas, R.DeVries, B.G.Harvey, D.Hendrie, J.Mahoney, J.Sherman, J.Steyaert, M.S.Zisman Anomaly in α-Scattering from 6Li between 35 and 45 MeV NUCLEAR REACTIONS 6Li(α, α), (α, α'), E=34.75, 39.75, 45 MeV; measured angular distributions from 20° to 160° (cm), angular distributions analyzed with optical model, cut-off optical model, addition of the exchange contribution. Enriched target.
doi: 10.1016/0375-9474(75)90040-8
1975BE40 Phys.Rev. C12, 894 (1975) F.D.Becchetti, B.G.Harvey, D.Kovar, J.Mahoney, C.Maguire, D.K.Scott 208Pb(16O, 15O)209Pb Reaction NUCLEAR REACTIONS 208Pb(16O, 15O), E=139 MeV; measured σ(E(15O), θ). 209Pb levels deduced S.
doi: 10.1103/PhysRevC.12.894
1975SC04 Phys.Rev.Lett. 34, 895 (1975) D.K.Scott, B.G.Harvey, D.L.Hendrie, U.Jahnke, L.Kraus, C.F.Maguire, J.Mahoney, Y.Terrien, K.Yagi, N.K.Glendenning Interference between Direct and Indirect Modes in Two-Nucleon Transfer Reactions with Heavy Ions NUCLEAR REACTIONS 122Sn(16O, 18O), E=104 MeV; 122Sn(18O, 16O), E=99 MeV; measured σ(θ); deduced reaction mechanism.
doi: 10.1103/PhysRevLett.34.895
1974BE16 Phys.Rev. C9, 1543 (1974) F.D.Becchetti, D.G.Kovar, B.G.Harvey, D.L.Hendrie, H.Homeyer, J.Mahoney, W.von Oertzen, N.K.Glendenning Two-Proton-Transfer Reactions 208Pb(12C, 10Be)210Po and 208Pb(16O, 14C)210Po NUCLEAR REACTIONS 208Pb(12C, 10Be), (16O, 14C), E(12C)=78 MeV, E(16O)=104, 140 MeV; 209Bi(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104 MeV; measured σ(Eout, θ). 210Po levels deduced relative strengths.
doi: 10.1103/PhysRevC.9.1543
1974BE58 Phys.Rev. C10, 1846 (1974) F.D.Becchetti, B.G.Harvey, D.Kovar, J.Mahoney, M.S.Zisman (16O, 15N) and (12C, 11B) Reactions on 54Fe and 62Ni at E(16O) = 104 MeV And E(12C) = 78 MeV NUCLEAR REACTIONS 54Fe, 62Ni(16O, 15N), E=104 MeV; 54Fe, 62Ni(12C, 11B), E=78 MeV; measured σ(E(15N), θ), σ(E(11B), θ). 55Co, 63Cu levels deduced J, S.
doi: 10.1103/PhysRevC.10.1846
1974DE03 Phys.Rev.Lett. 32, 680 (1974) R.M.DeVries, M.S.Zisman, J.G.Cramer, K.-L.Liu, F.D.Becchetti, B.G.Harvey, H.Homeyer, D.G.Kovar, J.Mahoney, W.von Oertzen Observation of an Anomalous Angular Distribution in the Single-Nucleon - Transfer Reaction 12C(14N, 13N)13C at 100 MeV NUCLEAR REACTIONS 12C(14N, 13N), E=100 MeV; measured σ(E(13N), θ). 13C deduced levels, L.
doi: 10.1103/PhysRevLett.32.680
1974SC26 Phys.Rev.Lett. 33, 1343 (1974) D.K.Scott, B.G.Harvey, D.L.Hendrie, L.Kraus, C.F.Maguire, J.Mahoney, Y.Terrien, K.Yagi Spectroscopy of Exotic Nuclei Using Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 26Mg(11B, 11C), (11B, 13N), (11B, 8B), 28Si(11B, 8B), E=86 MeV; measured σ; deduced Q. 26Mg deduced mass excess.
doi: 10.1103/PhysRevLett.33.1343
1973HE05 Phys.Rev.Lett. 30, 571 (1973) D.L.Hendrie, B.G.Harvey, J.R.Meriwether, J.Mahoney, J.-C.Faivre, D.G.Kovar Multipole Deformation of 238U NUCLEAR REACTIONS 238U(α, α), (α, α'), E=50 MeV; measured σ(θ). 238U deduced deformation parameters β(L).
doi: 10.1103/PhysRevLett.30.571
1973KO09 Phys.Rev.Lett. 30, 1075 (1973) D.G.Kovar, B.G.Harvey, F.D.Becchetti, J.Mahoney, D.L.Hendrie, H.Homeyer, W.von Oertzen, M.A.Nagarajan Evidence for Recoil Effects in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 208Pb(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104, 140 MeV; measured σ(E(11B), E(15N), θ); deduced recoil effects. 209Bi levels deduced S.
doi: 10.1103/PhysRevLett.30.1075
1973ZI04 Phys.Rev. C8, 1866 (1973) M.S.Zisman, F.D.Becchetti, B.G.Harvey, D.G.Kovar, J.Mahoney, J.D.Sherman Heavy-Ion-Induced Single-Nucleon Transfer Reactions in the Zr-Mo Region NUCLEAR REACTIONS 90,91,94Zr, 92Mo, 93Nb(16O, 15N), (16O, 15O), (16O, 16O'), E=104 MeV; 90Zr, 92Mo(12C, 11B), E=78 MeV; measured σ(E(15N), E(15O), E(11B), θ). 91,92,94,95Nb, 93Tc, 93,94Mo, 91,92,95Zr deduced levels, J, π, S, L.
doi: 10.1103/PhysRevC.8.1866
1972BE75 Phys.Rev. C6, 2215 (1972) F.D.Becchetti, D.G.Kovar, B.G.Harvey, J.Mahoney, B.Mayer, F.G.Puhlhofer Inelastic Scattering of 16O from 208Pb NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=104 MeV; measured σ(θ). 208Pb deduced levels, β, B(EL).
doi: 10.1103/PhysRevC.6.2215
1972KO32 Phys.Rev.Lett. 29, 1023 (1972) D.G.Kovar, F.D.Becchetti, B.G.Harvey, F.Puhlhofer, J.Mahoney, D.W.Miller, M.S.Zisman j Dependence of Heavy-Ion-Induced Reactions NUCLEAR REACTIONS 54Fe, 62Ni, 208Pb(16O, 15N), (12C, 11B), E=104, 78 MeV; measured σ ratios, σ(E(15N)), σ(E(11B)); deduced J-dependence. 55Co, 65Cu, 209Bi transitions deduced L.
doi: 10.1103/PhysRevLett.29.1023
1972SH21 Phys.Rev. C6, 1082 (1972) J.D.Sherman, B.G.Harvey, D.L.Hendrie, M.S.Zisman, B.Sorensen Strong and Weak 0+ Excitations in the 142Ce(p, t)140Ce and 140Ce(p, t)138Ce Reactions NUCLEAR REACTIONS 142Ce(p, t), 140Ce(p, t), E=30 MeV; measured σ(Et, θ). 138,140Ce deduced levels, L.
doi: 10.1103/PhysRevC.6.1082
1972ZI01 Phys.Rev. C5, 1031 (1972) High-Spin Levels of 92,93,94,95,96Nb and 94Tc Populated with (α, d) and (α, t) Reactions at 50 MeV NUCLEAR REACTIONS 90,91,92,94Zr, 92Mo(α, d), 91,92,94Zr(α, t), E=50 MeV; measured σ(Ed, θ), σ(Et, θ). 92,93,95Nb, 94,96Nb, 94Tc deduced levels, configurations.
doi: 10.1103/PhysRevC.5.1031
1971FA12 Ann.Phys.(N.Y.) 66, 905 (1971) H.Faraggi, A.Jaffrin, M.-C.Lemaire, M.C.Mermaz, J.-C.Faivre, J.Gastebois, B.G.Harvey, J.-M.Loiseaux, A.Papineau Evidence for Quartet Structures in the Nickel Region NUCLEAR REACTIONS 54,56Fe, 58,60,62,64Ni(16O, 12C), E=52, 48 MeV; measured σ(E(12C)). 58,60Ni, 62,64,66,68Zn deduced levels, quartet structure.
doi: 10.1016/0003-4916(71)90089-3
1971MC04 Phys.Lett. 34B, 289 (1971) R.L.McGrath, D.L.Hendrie, E.A.McClatchie, B.G.Harvey, J.Cerny The (d, 6Li) Reaction on Light Nuclei NUCLEAR REACTIONS 12C, 16O, 20Ne, 24,25Mg(d, 6Li), E=55 MeV; measured σ(E(6Li)).
doi: 10.1016/0370-2693(71)90607-1
1971ZI03 Phys.Rev. C4, 1809 (1971) High-Spin Proton States Observed in the Reactions 90Zr(α, t)91Nb and 92Mo(α, t)93Tc at 50 MeV NUCLEAR REACTIONS 90Zr(α, t), 92Mo(α, t), E=50 MeV; measured σ(Et, θ), Q. 91Nb, 93Tc deduced levels, L(p), S.
doi: 10.1103/PhysRevC.4.1809
1970FA05 Phys.Rev.Lett. 24, 1188 (1970) J.-C.Faivre, H.Faraggi, J.Gastebois, B.G.Harvey, M.-C.Lemaire, J.-M.Loiseaux, M.C.Mermaz, A.Papineau Experimental Evidence for Low-Lying Many-Quasiparticle States in Nickel Isotopes NUCLEAR REACTIONS 54,56Fe(16O, 12C), E=48 MeV; measured σ(E(12C)). 58,60Ni deduced low-lying 4p-2h states.
doi: 10.1103/PhysRevLett.24.1188
1970ZI03 Phys.Rev. C2, 1271 (1970) M.S.Zisman, E.A.McClatchie, B.G.Harvey 14N(α, d)16O Reaction at 40 MeV NUCLEAR REACTIONS 14N(α, d), E=40 MeV; measured σ(Ed, θ). 16O deduced levels, level-width, T.
doi: 10.1103/PhysRevC.2.1271
1969GA15 Nuovo Cimento 61B, 177 (1969) I.Gabrielli, B.G.Harvey, D.L.Hendrie, J.Mahoney, J.R.Meriwether, J.Valentin Scattering of Alpha-Particles by 55Mn NUCLEAR REACTIONS 55Mn(α, α), (α, α'), E=50 MeV; measured σ(Eα', θ); deduced optical model parameters. 55Mn deduced levels, J, π, B(E2), B(E3).
doi: 10.1007/BF02711705
1969LU07 Phys.Rev. 186, 1086 (1969) C.C.Lu, M.S.Zisman, B.G.Harvey High-Spin States of Configuration (1d5/2)2(5+, 0) and (1g9/2)2(9+, 0) Strongly Populated by the (α, d) Reaction NUCLEAR REACTIONS 13,14C, 15N, 20Ne(α, d), E = 40.1, 46, 45.4, 44.5 MeV; measured σ(Ed, θ). 15,16N, 17O, 22Na deduced levels, J, π, configuration. 52Cr, 54,56Fe, 58,60,62Ni, 64,66,68Zn(α, d), E = 50 MeV; measured σ(Ed, θ). 54Mn, 56,58Co, 60,62,64Cu, 66,68,70Ga deduced levels, J, π, configurations.
doi: 10.1103/PhysRev.186.1086
1968CH32 Nucl.Phys. A122, 481(1968) G.Chenevert, I.Halpern, B.G.Harvey, D.L.Hendrie The Evaporation of α-Particles from Heavy Nuclei NUCLEAR REACTIONS 181Ta, 197Au, 208Pb(α, α'); E=50, 65, 90 MeV; measured σ(Eα', θ). Interpreted low-energy portion of backward angle spectra in terms of statistical theory.
doi: 10.1016/0375-9474(68)90573-3
1968GL03 Phys.Rev.Letters 21, 918(1968); Erratum Phys.Rev.Letters 21, 1220(1968) C.Glashausser, B.G.Harvey, D.L.Hendrie, J.Mahoney, E.A.McClatchie, J.Saudinos Excitation of Single-Neutron-Hole States in Pb207 by Inelastic Proton Scattering at 20.2 MeV NUCLEAR REACTIONS 207Pb(p, p'), E=20.2 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.21.918
1968HE24 Phys.Letters 26B, 127 (1968) D.L.Hendrie, N.K.Glendenning, B.G.Harvey, O.N.Jarvis, H.H.Duhm, J.Saudinos, J.Mahoney Determination of Y40 and Y60 Components in the Shapes of Rare Earth Nuclei NUCLEAR REACTIONS 152,154Sm, 158Gd, 166Er, 174,176Yb, 178Hf(α, α'), E=50 MeV; measured σ(θ). Deduced deformation parameters.
doi: 10.1016/0370-2693(68)90502-9
1968LU04 UCRL-17989, p.61 (1968) C.-C.Lu, M.S.Zisman, B.G.Harvey High Spin Proton-Neutron Two-Particle Levels in the Medium-Mass (54 < a < 70) Region NUCLEAR STRUCTURE 54Mn, 66Ga, 68Ga; measured not abstracted; deduced nuclear properties.
1968LU05 Phys.Lett. 27B, 217 (1968) C.C.Lu, M.S.Zisman, B.G.Harvey Proton-Neutron Two-Particle Excited States of the (1g9/2)2 9+ Configuration NUCLEAR REACTIONS 52Cr, 54,56Fe, 58,60,62Ni, 64,66,68Zn(α, d), E=50 MeV; measured σ(Ed, θ). 54Mn, 56,58Co, 60,62,64Cu, 66,68,70Ga deduced level of (g9/2)2 configuration. Enriched targets.
doi: 10.1016/0370-2693(68)90276-1
1968MA29 Nucl.Phys. A117, 161(1968) N.F.Mangelson, B.G.Harvey, N.K.Glendenning Spectroscopy of 14N by Use of the 12C(3He, p)14N Reaction NUCLEAR REACTIONS 12C(3He, p), E=20.1 MeV; measured σ(Ep, θ). 14N levels deduced J, π, L. Natural target.
doi: 10.1016/0375-9474(68)90868-3
1968MA33 Nucl.Phys. A119, 79(1968) Erratum Nucl.Phys. A127, 693(1969) N.F.Mangelson, B.G.Harvey, N.K.Glendenning Study of 18F by Use of (3He, p) and (α, d) Reactions NUCLEAR REACTIONS 16O(3He, p), E=19.8 MeV; measured σ(Ep, θ). 16O(α, d), E=40.3 MeV; measured σ(Ed, θ). 18F deduced levels, J, π, L. Natural target.
doi: 10.1016/0375-9474(68)90807-5
1967HA05 Phys.Letters 24B, 43 (1967) B.G.Harvey, D.L.Hendrie, O.N.Jarvis, J.Mahoney, J.Valentin Multiple Nuclear Excitation of Rotational Levels in 152Sm and 154Sm NUCLEAR STRUCTURE 152Sm, 154Sm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90334-6
1967JA08 Nucl.Phys. A102, 625 (1967) O.N.Jarvis, B.G.Harvey, D.L.Hendrie, J.Mahoney The Inelastic Scattering of 17.8 MeV Protons from 58Ni, 60Ni and 120Sn And the Determination of Spin and Parity Assignments for 58Ni and α-Particle Scattering NUCLEAR REACTIONS 58Ni, 60Ni, 120Sn(p, p'), E=17.8 MeV; measured σ(Ep', θ); deduced optical-model. 58Ni(α, α'), E=50.2 MeV; measured σ(Eα', θ). 58,60Ni, 120Sn deduced deformation parameters. 58Ni deduced J, π.
doi: 10.1016/0375-9474(67)90399-5
1966HA19 Phys.Rev. 146, 712 (1966) B.G.Harvey, J.R.Meriwether, J.Mahoney, A.Bussiere de Nercy, D.J.Horen Scattering of 40.5-MeV Alpha Particles by C12, C13, N14, N15, O16, and O18 NUCLEAR STRUCTURE 18O, 12C, 16O, 14N, 13C, 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.146.712
1966ME07 Phys.Rev. 146, 804 (1966) J.R.Meriwether, I.Gabrielli, D.L.Hendrie, J.Mahoney, B.G.Harvey Scattering of Alpha Particles by Cr52, Cr53, and V51 NUCLEAR STRUCTURE 51V, 52Cr, 53Cr; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.146.804
1966RI04 Phys.Rev. 141, 1021 (1966) E.Rivet, R.H.Pehl, J.Cerny, B.G.Harvey Investigation of High Spin Levels Preferentially Populated by the (α, d) Reaction NUCLEAR STRUCTURE 14N, 16O, 26Al, 28Al, 12C, 30P, 42K, 42Sc, 18F, 22Na, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.141.1021
1966VA22 UCRL-16580, p.133 (1966) J.Valentin, I.Garbrielli, B.G.Harvey, D.L.Hendrie, J.Mahoney, J.R.Meriwether Inelastic Scattering of α Particles on Fe56 NUCLEAR STRUCTURE 56Fe; measured not abstracted; deduced nuclear properties.
1965BU05 Phys.Letters 16, 296 (1965) A.Bussiere, N.K.Glendenning, B.G.Harvey, J.Mahoney, J.R.Meriwether, D.J.Horen Octupole States in 15N and 16O NUCLEAR STRUCTURE 16O, 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90859-0
1965HA27 Nucl.Phys. 70, 305 (1965) B.G.Harvey, J.R.Meriwether, A.Bussiere, D.J.Horen Excitation of Collective Levels in Cu63 by 50 MeV α-Scattering NUCLEAR REACTIONS 62Ni, 63Cu(α, α'), E = 50 MeV; measured σ (Eα', θ). 62Ni, 63Cu deduced B(E2). Enriched targets.
doi: 10.1016/0029-5582(65)90526-2
1965HO08 Nucl.Phys. 72, 97 (1965) D.J.Horen, J.R.Meriwether, B.G.Harvey, A.Bussiere de Nercy, J.Mahoney Phase Variation in the Scattering of Alpha Particles by Ni58,62 NUCLEAR REACTIONS 58Ni(α, α'), 62Ni(α, α'), E = 25, 33, 50, 85, 100 MeV; measured σ(E;Eα', θ(α')). 58,62Ni deduced B(EL), matrix elements. Enriched targets. 129Te [from 128Te(n, γ)]; measured Eγ, Iγ, γγ-coin. 129I deduced levels. Enriched target.
doi: 10.1016/0029-5582(65)90628-0
1965PE03 Phys.Rev. 137, B114 (1965) R.H.Pehl, E.Rivet, J.Cerny, B.G.Harvey C12(α, d)N14 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B114
1965PE17 Phys.Rev. 140, B605 (1965) R.H.Pehl, J.Cerny, E.Rivet, B.G.Harvey (d, α) Reactions on C12, N14, and O16 Induced by 24-MeV Deuterons NUCLEAR STRUCTURE 16O, 14N, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B605
1965SP01 Phys.Letters 14, 116 (1965) Inelastic Scattering of 50.9-MeV Alpha Particles from Ca40 NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.14.316
1965SP02 Phys.Rev.Letters 14, 316 (1965) Inelastic Scattering of 50.9-MeV Alpha Particles from Ne20 NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.14.316
1964HA16 Nucl.Phys. 52, 465 (1964) B.G.Harvey, E.J-M.Rivet, A.Springer, J.R.Meriwether, W.B.Jones, J.H.Elliott, P.Darriulat Scattering of 65 MeV Helium Ions from O16 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90708-4
1964HA24 UCRL-11213, p.77(1964) B.G.Harvey, D.J.Horen, J.R.Meriwether The Scattering of Alpha Particles from Cu63 and Ni62 NUCLEAR STRUCTURE 63Cu, 62Ni; measured not abstracted; deduced nuclear properties.
1964ME06 Phys.Letters 11, 299 (1964) J.R.Meriwether, A.Bussiere de Nercy, B.G.Harvey, D.J.Horen Energy Variation of the Phase Rule in Alpha Particle Scattering NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90337-3
1964RI03 UCRL-11213, p.71 (1964) E.J-M.Rivet, J.Cerny, B.G.Harvey, R.H.Pehl, J.Haag The Formation of Strongly Populated High Spin Levels in (α, d) Reactions NUCLEAR STRUCTURE 42K, 42Sc, 26Al, 22Na; measured not abstracted; deduced nuclear properties.
1963CE02 Phys.Letters 7, 67 (1963) J.Cerny, R.H.Pehl, E.Rivet, B.G.Harvey Investigation of Isobaric-Spin Conservation in the O16(d, α)N14 Reaction Using a High Resolution Semiconductor E-(dE/dx) System NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90445-1
1963HA50 Bull.Am.Phys.Soc. 8, No.8, 612, N8 (1963) B.G.Harvey, J.R.Meriwether, D.J.Horen Excitation of Collective Levels in Cu63 by 50-MeV α Scattering NUCLEAR STRUCTURE 63Cu; measured not abstracted; deduced nuclear properties.
1962CE01 Nuclear Phys. 29, 120 (1962) (α, d) Reactions on Odd Targets NUCLEAR STRUCTURE 6Li, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90171-2
1962HA40 Nuclear Phys. 39, 160 (1962) B.G.Harvey, J.Cerny, R.H.Pehl, E.Rivet Levels Involving A (d5/2)52 State in Light Nuclei
doi: 10.1016/0029-5582(62)90383-8
1962HA48 UCRL-10624, p.181 (1962) B.G.Harvey, J.Cerny, R.H.Pehl, E.J.M.Rivet Two-Nucleon Stripping Reactions NUCLEAR STRUCTURE 42Sc, 42K; measured not abstracted; deduced nuclear properties.
1961CE02 Bull.Am.Phys.Soc. 6, No.6, 507, E11 (1961) J.Cerny, N.K.Glendenning, B.G.Harvey, R.H.Pehl, E.Rivet Analysis of the Two-Nucleon Stripping Reaction C12(He3, p)N14 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961CE04 UCRL-10023, p.114 (1961) The Reaction N15(α, d)O17 NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
1961PE24 UCRL-10023, p.121 (1961) Investigation of Isobaric-Spin Conservation in the O16(d, α)N14 Reaction using a High-Resolution Semiconductor E-dE/dx System
1960CE01 Bull.Am.Phys.Soc. 5, No.7, 493, C3 (1960) Reactions Li6(α, d)Be8 and Li7(α, d)Be9 with 48-MeV Helium Ions NUCLEAR STRUCTURE 9Be, 8Be; measured not abstracted; deduced nuclear properties.
1960DO07 Phys.Rev. 119, 218 (1960) P.F.Donovan, B.G.Harvey, W.H.Wade Recoil Studies of Heavy Element Nuclear Reactions. I. NUCLEAR STRUCTURE 210At, 208Po, 209At; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.119.218
1960HA10 Bull.Am.Phys.Soc. 5, No.4, 230, C10 (1960) Deuteron Spectra from Bombardment of C12, N14, and N15 with 48-MeV Helium Ions NUCLEAR STRUCTURE 17O, 16O, 14N; measured not abstracted; deduced nuclear properties.
1960HA25 UCRL-9093, 15 (1960) NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1960HA31 Bull.Am.Phys.Soc. 5, No.7, 493, C4 (1960) Comparison of the Reactions C12(He3, n)N14 and C12(α, d)N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1960HA32 Phys.Rev. 120, 2162 (1960) Reaction C12(α, d)N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.2162
1957AM47 Phys.Rev. 106, 553 (1957) S.Amiel, A.Chetham-Strode, Jr., G.R.Choppin, A.Ghiorso, B.G.Harvey, L.W.Holm, S.G.Thompson Production and Properties of the Nuclides Fermium-250, 251, and 252
doi: 10.1103/PhysRev.106.553
1957HA08 Can.J.Phys.35, 258 (1957) B.G.Harvey, H.G.Jackson, T.A.Eastwood, G.C.Hanna The Energy of Alpha Particles from U234, U238, and Th232
doi: 10.1139/p57-030
1956AL40 Priv.Comm., quoted by 1956HO54 unpublished (1956) R.G.Albridge, B.G.Harvey, J.M.Hollander
1956AL41 Priv.Comm., quoted by 1956Ho54, unpublished (1956) R.G.Albridge, B.G.Harvey, J.M.Hollander RADIOACTIVITY 242mAm; measured not abstracted. 242Cm deduced level.
1956CH43 Phys.Rev. 102, 747 (1956) A.Chetham-Strode, Jr., G.R.Choppin, B.G.Harvey Mass Assignment of the 44-Minute Californium-245 and the New Isotope Californium-244
doi: 10.1103/PhysRev.102.747
1956CH81 Phys.Rev. 102, 766 (1956) G.R.Choppin, B.G.Harvey, D.A.Hicks, J.Ise, R.V.Pyle Prompt Neutrons from the Spontaneous Fission of Fermium-254 RADIOACTIVITY 254Fm(SF); measured products; deduced miscellaneous fission parameters. Data were imported from EXFOR entry 13649.
doi: 10.1103/PhysRev.102.766
1956HA80 Phys.Rev. 104, 1315 (1956) B.G.Harvey, A.Chetham-Strode, A.Ghiorso, G.R.Choppin, S.G.Thompson New Isotopes of Einsteinium
doi: 10.1103/PhysRev.104.1315
1955AS42 Phys.Rev. 100, 137 (1955) F.Asaro, F.S.Stephens, B.G.Harvey, I.Perlman Complex Alpha and Gamma Spectra of Cf250,252
doi: 10.1103/PhysRev.100.137
1955AS64 Priv.Comm., quoted by 1964Hy02, unpublished (1955) F.Asaro, B.G.Harvey, F.S.Stephens, Jr., I.Perlman
1955CH30 Phys.Rev. 98, 1519 (1955) G.R.Choppin, B.G.Harvey, S.G.Thompson, A.Ghiorso Nuclear Properties of 100256
doi: 10.1103/PhysRev.98.1519
1955GH02 Phys.Rev. 98, 1518 (1955) A.Ghiorso, B.G.Harvey, G.R.Choppin, S.G.Thompson, G.T.Seaborg New Element Mendelevium, Atomic Number 101 NUCLEAR REACTIONS 253Es(He, X)256Md, E=48 MeV; measured reaction products, Eα, Iα; deduced a new Z=101 element in recognition of the pioneering role of the great Russian chemist, Dmitri Mendeleev, who was the first to use the periodic system of the elements to predict the chemical properties of undiscovered elements, a principle which has been the key to the discovery of the last seven transuranium (actinide) elements. RADIOACTIVITY 256Md(α); measured decay products, Eα, Iα; deduced T1/2.
doi: 10.2172/914464
1955HA35 Phys.Rev. 99, 337 (1955) B.G.Harvey, S.G.Thompson, G.R.Choppin, A.Ghiorso Nuclide 99254
doi: 10.1103/PhysRev.99.337
1954CH23 Phys.Rev. 94, 1080 (1954) G.R.Choppin, S.G.Thompson, A.Ghiorso, B.G.Harvey Nuclear Properties of Some Isotopes of Californium, Elements 99 and 100
doi: 10.1103/PhysRev.94.1080
1954GH12 Phys.Rev. 93, 257 (1954) A.Ghiorso, G.B.Rossi, B.G.Harvey, S.G.Thompson Reactions of U238 with Cyclotron-Produced Nitrogen Ions
doi: 10.1103/PhysRev.93.257
1954GH24 Phys.Rev. 94 1081 (1954) A.Ghiorso, S.G.Thompson, G.R.Choppin, B.G.Harvey New Isotopes of Americium, Berkelium and Californium
doi: 10.1103/PhysRev.94.1081
1954GH25 Phys.Rev. 95, 293 (1954) A.Ghiorso, S.G.Thompson, G.H.Higgins, B.G.Harvey, G.T.Seaborg Evidence for Subshell at N = 152 RADIOACTIVITY 244,246,248,249,250,252Cf, Pu, Am, Cm, Bk, Es, Fm(α); analyzed available data; deduced α-particle energy vs. mass number systematics, N=152 subshell.
doi: 10.1103/PhysRev.95.293
1954HA69 Phys.Rev. 95, 581 (1954) B.G.Harvey, H.P.Robinson, S.G.Thompson, A.Ghiorso, G.R.Choppin Some pile neutron cross sections of isotopes of americium, berkelium, californium, and element 99 NUCLEAR REACTIONS 243Am(n, γ), 249Bk, 249Cf(n, X), 249Cf(n, f), 249Cf(n, γ), 252Cf(n, γ), 254Cf(n, γ), 253Es(n, γ), 254Es(n, γ), E=0.0253 eV; measured products, 244Am, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12567.
doi: 10.1103/PhysRev.95.581
1954HA73 Phys.Rev. 93, 1129 (1954) B.G.Harvey, S.G.Thompson, A.Ghiorso, G.R.Choppin Further Production of Transcurium Nuclides by Neutron Irradiation RADIOACTIVITY 254Es, 253Cf(β-) [from 252Cf, 254Es(n, γ), E thermal]; measured decay products. 254Fm; deduced element 100. The Materials Testing Reactor (MTR).
doi: 10.1103/PhysRev.93.1129
1954TH01 Phys.Rev. 93, 908 (1954) S.G.Thompson, A.Ghiorso, B.G.Harvey, G.R.Choppin Transcurium Isotopes Produced in the Neutron Irradiation of Plutonium
doi: 10.1103/PhysRev.93.908
1952DE01 Phys.Rev. 85, 499 (1952) Preparation of Ra229 and Ac229
doi: 10.1103/PhysRev.85.499
1952HA68 Phys.Rev. 85, 482 (1952) The α-Half-Life of Am 241 RADIOACTIVITY 241Am(α); measured specific activity; deduced T1/2.
doi: 10.1103/PhysRev.85.482
1951HA87 Phys.Rev. 81, 466 (1951) G.C.Hanna, B.G.Harvey, N.Moss, P.R.Tunnicliffe Spontaneous Fission in Cm242
doi: 10.1103/PhysRev.81.466
1951HA88 Phys.Rev. 81, 486 (1951) The Neutron Capture Cross Section Of Am241 NUCLEAR REACTIONS 241Am(n, X), E=0.0253 eV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12582.
doi: 10.1103/PhysRev.81.486
1951HA89 Phys.Rev. 81, 893 (1951) G.C.Hanna, B.G.Harvey, N.Moss, P.R.Tunnicliffe Fission In Am242 NUCLEAR REACTIONS 238Pu(n, f), 241Am(n, f), 242Am(n, X), 242Am(n, f), 242Cm(n, f), E=0.0253 eV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12496.
doi: 10.1103/PhysRev.81.893
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