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NSR database version of April 11, 2024.

Search: Author = I.D.Proctor

Found 20 matches.

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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0052.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0602.


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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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1971TR06      Phys.Lett. 35B, 570 (1971)

G.F.Trentelman, I.D.Proctor

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
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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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