NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = I.Proctor Found 21 matches. 1995MC05 Nucl.Instrum.Methods Phys.Res. B99, 541 (1995) J.E.McAninch, G.S.Bench, S.P.H.T.Freeman, M.L.Roberts, J.R.Southon, J.S.Vogel, I.D.Proctor PXAMS - Projectile X-Ray AMS: X-ray yields and applications NUCLEAR REACTIONS Ca, C, O, Ti(28Si, X), E=56 MeV; Cu(56Fe, X), Zn(58Ni, X), (Ge, X), E=102 MeV; 89Y(80Se, X), E=100, 102 MeV; Rh(92Mo, X), Ag(106Pd, X), E=106 MeV; measured X-ray yields. ATOMIC PHYSICS Ca, C, O, Ti(28Si, X), E=56 MeV; Cu(56Fe, X), Zn(58Ni, X), (Ge, X), E=102 MeV; 89Y(80Se, X), E=100, 102 MeV; Rh(92Mo, X), Ag(106Pd, X), E=106 MeV; measured X-ray yields.
doi: 10.1016/0168-583X(94)00633-4
1986BA39 Phys.Rev. C34, 1110 (1986) R.W.Bauer, J.A.Becker, I.D.Proctor, D.J.Decman, R.G.Lanier, J.A.Cizewski (p, t) Reaction on Even-Mass Cadmium Nuclei: Test for the admixture of intruder configurations in the ground states NUCLEAR REACTIONS 106,108,110,112,114,116Cd(p, t), E=26 MeV; measured σ(θ); deduced model parameters. 104,106,108,110,112,114Cd level deduced enhancement factor, no intruder configuration admixture. Split-pole spectrograph, position sensitive detector. DWBA calculation.
doi: 10.1103/PhysRevC.34.1110
1982HA02 Phys.Rev. C25, 189 (1982) L.F.Hansen, I.D.Proctor, D.W.Heikkinen, V.A.Madsen Nuclear Deformation in the Actinide Region by Proton Inelastic Scattering NUCLEAR REACTIONS 232Th, 238U(p, p), (p, p'), E=26 MeV; measured σ(θ); deduced potential multipole moments. 232Th, 238U deduced β2, β4. Coupled-channels analysis.
doi: 10.1103/PhysRevC.25.189
1981LA02 Phys.Lett. 99B, 23 (1981) R.G.Lanier, G.L.Struble, L.G.Mann, W.Stoffl, I.C.Oelrich, J.Scheerer, I.D.Proctor, D.W.Heikkinen, R.H.Howell Evidence for a Strongly Deformed Prolate Shape at N=87 from 154Eu and 152Eu(p, t) Reactions NUCLEAR REACTIONS 152,154Eu(p, t), E=20 MeV; measured σ(Et, θ). 150Eu deduced prolate structure. 150,152Eu deduced levels, J, π, L, rotational bands, Nilsson assignments, rotational parameter. Q3D spectrograph. DWBA analysis.
doi: 10.1016/0370-2693(81)90796-6
1980LA11 Phys.Rev. C22, 51 (1980) R.G.Lanier, G.L.Struble, L.G.Mann, I.C.Oelrich, I.D.Proctor, D.W.Heikkinen Evidence for Nuclear Shape Coexistence at N = 88: 152Eu(d, p) and (d, t) Reactions NUCLEAR REACTIONS 152Eu(d, p), (d, t), E=20 MeV; measured Ep, Et, σ(θ). 153,151Eu deduced levels, J, π, Nilsson assignments, shape.
doi: 10.1103/PhysRevC.22.51
1979LA11 Phys.Rev. C20, 1279 (1979) R.G.Lanier, L.G.Mann, G.L.Struble, I.D.Proctor, D.W.Heikkinen Proton Inelastic Scattering at 12 MeV on 154Eu NUCLEAR REACTIONS 154Eu(p, p'), E=12 MeV; measured σ(Ep, θ). 154Eu deduced levels, J, π, β2, β4. Isotopically enriched radioactive target. Split-pole spectrograph; adiabatic coupled-channel analysis. Assigned Nilsson configuration.
doi: 10.1103/PhysRevC.20.1279
1979MA08 Phys.Rev. C19, 1191 (1979) L.G.Mann, J.B.Carlson, R.G.Lanier, G.L.Struble, W.M.Buckley, D.W.Heikkinen, I.D.Proctor, R.K.Sheline 181Ta(p, 2nγ)180W Reaction NUCLEAR REACTIONS 181Ta(p, 2nγ), E=16 MeV; measured Eγ, Iγ, γγ-coin, T1/2, γ(θ). 180W deduced levels, E, J, π, K.
doi: 10.1103/PhysRevC.19.1191
1978LA10 Phys.Rev. C18, 1609 (1978) R.G.Lanier, L.G.Mann, G.L.Struble, I.D.Proctor, D.W.Heikkinen Deformation Change at N = 89: Proton Inelastic Scattering at 12 MeV on 151,152,153Eu NUCLEAR REACTIONS 151,152,153Eu(p, p'), E=12 MeV; measured σ(Ep', θ). 151,152,153Eu deduced levels, J, π, β2, β4. 152Eu deduced Nilsson configurations. Split-pole spectrograph, DWBA, coupled channel analyses. Isotopically enriched, radioactive targets.
doi: 10.1103/PhysRevC.18.1609
1978LA15 Phys.Lett. 78B, 217 (1978) R.G.Lanier, G.L.Struble, L.G.Mann, I.D.Proctor, D.W.Heikkinen On the Stability of a Ground-State Rotational Structure for the Transitional Nucleus 152Eu NUCLEAR REACTIONS 151,153Eu(p, p'), E=12 MeV; measured σ(Ep'). 152Eu(p, p'), E=12 MeV; measured σ(Ep', θ). 152Eu deduced levels, influence of h11/2 orbital.
doi: 10.1016/0370-2693(78)90009-6
1975HA13 Nucl.Phys. A241, 285 (1975) R.C.Haight, I.D.Proctor, H.F.Lutz, W.Bartolini The 30Si(p, d)29Si and 30Si(p, t)28Si Reactions at 27 MeV NUCLEAR REACTIONS 30Si(p, d), 30Si(p, t), E=27 MeV; measured σ(Ed, θ), σ(Et, θ). 29Si deduced levels, J, π, S. 28Si deduced levels, L, π, enhancement ratios. Enriched target.
doi: 10.1016/0375-9474(75)90318-8
1974LU07 Nucl.Phys. A231, 365 (1974) H.F.Lutz, D.W.Heikkinen, W.Bartolini, I.D.Proctor Coupled-Channel Analysis of Proton Inelastic Scattering by 48Ti NUCLEAR REACTIONS 48Ti(p, p), (p, p'), E=16.5, 18.0, 20.0, 22.0, 24.0 MeV; measured σ(Ep, θ), σ(Ep', θ). 48Ti deduced levels, deformation parameters βλ. Enriched target. Coupled-channel calculation.
doi: 10.1016/0375-9474(74)90501-6
1974NO07 Nucl.Instrum.Methods 115, 189 (1974) J.A.Nolen, Jr., G.Hamilton, E.Kashy, I.D.Proctor Measuring Nuclear Excitation Energies and Q-Values with a Cyclotron-Magnetic Spectrograph System NUCLEAR REACTIONS 24Mg, 12C(p, p'), (p, d); 24Mg(p, t); measured Q. 11,12C, 24Mg deduced levels.
doi: 10.1016/0029-554X(74)90446-7
1973BE09 Phys.Lett. 43B, 117 (1973) W.Benenson, E.Kashy, I.D.Proctor, B.M.Preedom The Mass of 29S NUCLEAR REACTIONS 32S(3He, 6He), E=70 MeV; measured Q. 29S deduced mass excess.
doi: 10.1016/0370-2693(73)90423-1
1973BE14 Phys.Rev. C7, 1143 (1973) W.Benenson, E.Kashy, I.D.Proctor Mass-25 Isobaric Multiplets NUCLEAR REACTIONS 27Al(p, t), (p, 3He), E=40 MeV; 26Mg(p, d), E=36 MeV; 26Mg(d, 3He), E=24 MeV. Measured Q, σ(Et), σ(E(3He)), σ(Ed). Coefficients of isobaric-mass-doublet equation. 25Al, 25Mg deduced levels.
doi: 10.1103/PhysRevC.7.1143
1973BE23 Phys.Rev. C8, 210 (1973); Erratum Phys.Rev. C8, 1968 (1973) W.Benenson, E.Kashy, I.D.Proctor Isobaric Mass Quartets in the Mass-21 and Mass-37 Nuclei NUCLEAR REACTIONS 24Mg, 40Ca(3He, 6He), E=70.7 MeV; measured σ(E(6He)), Q. 39K(p, t), (p, 3He), E=40.1, 42.7 MeV; measured σ(Et, E(3He)), Q. 21Mg, 37Ca, 37K, 37Ar deduced levels.
doi: 10.1103/PhysRevC.8.210
1973KA16 Phys.Rev. C7, 2251 (1973) E.Kashy, W.Benenson, I.D.Proctor, P.Hauge, G.Bertsch Three-Neutron Pickup Reaction on 13C NUCLEAR REACTIONS 13C(3He, 6He), E=70.3 MeV; measured σ(E(3He), θ).
doi: 10.1103/PhysRevC.7.2251
1972BE12 Phys.Rev. C5, 1426 (1972) W.Benenson, J.Dreisbach, I.D.Proctor, G.F.Trentelman, B.M.Preedom Energy Levels of 25Si from the Reaction 28Si(3He, 6He)25Si at 70.4 MeV NUCLEAR REACTIONS 28Si(3He, 6He), E=70.4 MeV; measured σ(E(6He)), Q. 25Si deduced levels, ground-state mass excess.
doi: 10.1103/PhysRevC.5.1426
1972PR10 Phys.Rev.Lett. 29, 434 (1972) I.D.Proctor, W.Benenson, J.Dreisbach, E.Kashy, G.F.Trentelman, B.M.Preedom New Proton-Rich Nuclei in the 1 f7/2 Shell NUCLEAR REACTIONS 54Fe, 46Ti, 50Cr, 58Ni(3He, 6He), E=65-75 MeV; measured Q, σ(E(6He)). 43Ti, 51Fe, 47Cr, 55Ni deduced masses.
doi: 10.1103/PhysRevLett.29.434
1971TR06 Phys.Lett. 35B, 570 (1971) The Mass of 25Si and the Isobaric Multiplet Mass Equation NUCLEAR REACTIONS 28Si(3He, 6He), E=70 MeV; measured Q, σ(E(6He)). 25Si deduced mass excess.
doi: 10.1016/0370-2693(71)90289-9
1970HI06 Phys.Rev.Lett. 25, 829 (1970) R.A.Hinrichs, R.Sherr, G.M.Crawley, I.Proctor Anomalous L = 1 Shapes of Angular Distribution for (3He, t) Transitions to 0+ Antianalog States in 64,66Ga and 40K NUCLEAR REACTIONS 40Ar, 64,66Zn(3He, t), E=35 MeV; measured σ(θ). 40K, 64,66Ga deduced transitions, antianalog states.
doi: 10.1103/PhysRevLett.25.829
1969PA09 Phys.Rev. 182, 1104 (1969) R.A.Paddock, S.M.Austin, W.Benenson, I.D.Proctor, F.S.Amant Gamma Rays from Protons on 10B, and the Excitation Energy of the First Excited State of 10C NUCLEAR REACTIONS 10B(p, nγ), (p, p'γ), E=11.4 MeV; measured Eγ. 10B, 10C deduced levels. Enriched 10B target, Ge(Li) detector.
doi: 10.1103/PhysRev.182.1104
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