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NSR database version of April 11, 2024.

Search: Author = W.A.Gillespie

Found 19 matches.

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1979VA03      J.Phys.(London) G5, 315 (1979)

C.W.E.van Eijk, J.Wijnhorst, M.A.Popelier, W.A.Gillespie

The Difference in Nuclear Charge Radius between 110,112,114,116Cd

NUCLEAR STRUCTURE 110,112,114,116Cd; measured K X-ray isotope shift; deduced rms charge radii for isotope pairs. Compared with optical isotopic shift.

doi: 10.1088/0305-4616/5/2/018
Citations: PlumX Metrics


1978AR07      J.Phys.(London) G4, 961 (1978)

R.G.Arthur, R.P.Singhal, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, M.W.S.Macauley

Vibrational States in 108Pd Studied by Elastic and Inelastic Electron Scattering

NUCLEAR REACTIONS 108Pd(e, e), E=21-121 MeV; measured σ(E). 108Pd levels deduced form factors, quadrupole moment, B(λ).

doi: 10.1088/0305-4616/4/6/023
Citations: PlumX Metrics


1977BR16      J.Phys.(London) G3, 821 (1977)

S.W.Brain, A.Johnstons, W.A.Gillespie, E.W.Lees, R.P.Singhal

The Ground-State Charge Distribution of the Silicon Isotopes and the Excited States of 28Si, 30Si

NUCLEAR REACTIONS 28,29,30Si(e, e'), E=18.5-117.1 MeV; measured σ(E, θ). 28,30Si deduced rms radii, B(λ). 29Si deduced rms radii.

doi: 10.1088/0305-4616/3/6/013
Citations: PlumX Metrics


1977BR35      J.Phys.(London), G3, 681 (1977)

S.W.Brain, A.Johnston, W.A.Gillespie, E.W.Lees, R.P.Singhal

Inelastic Electron Scattering from 29Si

NUCLEAR REACTIONS 29Si(e, e'), E=63-117 MeV; measured σ(E;θ). 29Si deduced levels, B(λ). Enriched target, resolution=0.16%, DWBA analysis.

doi: 10.1088/0305-4616/3/5/014
Citations: PlumX Metrics


1977GI13      J.Phys.(London) G3, L-169 (1977)

W.A.Gillespie, M.W.S.Macauley, A.Johnston, E.W.Lees, R.P.Singhal

B(E2) and Q21+ Measurements in the Even-Mass Cd Isotopes

NUCLEAR REACTIONS 110,112,114,116Cd(e, e'), E=68, 112 MeV; measured σ(θ). 110,112,114,116Cd deduced quadrupole moment, B(E2). Separated targets, resolution 0.15%, DWBA analysis, anharmonic vibrational model.

doi: 10.1088/0305-4616/3/8/005
Citations: PlumX Metrics


1977MA42      J.Phys.(London) G3, 1717 (1978)

M.W.S.Macauley, R.P.Singhal, R.G.Arthur, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight

An Experimental and Theoretical Study of the Low-Lying States of 15N

NUCLEAR REACTIONS 15N(e, e'), E=60-120 MeV; measured σ(E, θ). 15N deduced form factors, B(λ). Separated isotope gas target. Shell model, DWBA analysis.

doi: 10.1088/0305-4616/3/12/011
Citations: PlumX Metrics


1977SI02      Nucl.Phys. A279, 29 (1977)

R.P.Singhal, A.Johnston, W.A.Gillespie, E.W.Lees

Inelastic Scattering of Electrons from 27Al

NUCLEAR REACTIONS 27Al(e, e'), E=62-112 MeV; measured σ. 27Al deduced B(E2), transition radius. Intermediate-coupling model, large-basis shell model.

doi: 10.1016/0375-9474(77)90418-3
Citations: PlumX Metrics


1976GI07      J.Phys.(London) G2, 185 (1976)

W.A.Gillespie, R.P.Singhal, S.W.Brain, A.Johnston, E.W.Lees

Excitation of Vibrational States in 114Cd by Inelastic Electron Scattering

NUCLEAR REACTIONS 114Cd(e, e'), E=68-112 MeV; measured σ(E, θ). 114Cd levels deduced form-factors, B(λ), quadrupole moment, β. Anharmonic model.

doi: 10.1088/0305-4616/2/3/010
Citations: PlumX Metrics


1976LE07      J.Phys.(London) G2, 105 (1976)

E.W.Lees, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, R.P.Singhal

Elastic Electron Scattering from the Stable Isotopes of Magnesium

NUCLEAR REACTIONS 24,25,26Mg(e, e'), E=22.9-119.7 MeV; measured σ(E, θ). 24,25,26Mg deduced rms radii, form factors. DWBA analysis. Enriched targets.

doi: 10.1088/0305-4616/2/2/007
Citations: PlumX Metrics


1976LE11      J.Phys.(London) G2, 341 (1976)

E.W.Lees, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, R.P.Singhal

Inelastic Electron Scattering from 25Mg

NUCLEAR REACTIONS 25Mg(e, e'), E=61.9-119.3 MeV; measured σ(E, θ). 25Mg levels deduced radial parameters, B(E2), form factors. DWBA analysis, Nilsson model comparison, enriched target.

doi: 10.1088/0305-4616/2/5/010
Citations: PlumX Metrics


1976MA30      J.Phys.(London) G2, L35 (1976)

M.W.S.Macauley, R.P.Singhal, R.G.Arthur, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight

The 6.32 MeV Excitation in 15N: Is it a Single-Particle Transition (Question)

NUCLEAR REACTIONS 15N(e, e'), E=60-120 MeV; measured σ(E, θ). 15N level deduced form factors, effective charge. DWBA, shell model analysis. Enriched target.

doi: 10.1088/0305-4616/2/3/004
Citations: PlumX Metrics


1975LE02      J.Phys.(London) G1, L13 (1975)

E.W.Lees, C.S.Curran, S.W.Brain, W.A.Gillespie, A.Johnston, R.P.Singhal

The Ground State Band of 25Mg Studied by Electron Scattering

NUCLEAR REACTIONS 25Mg(e, e'), E=61.9-119.3 MeV; measured σ(E, Ee', θ). 25Mg transitions deduced B(E2).

doi: 10.1088/0305-4616/1/2/001
Citations: PlumX Metrics


1975SI21      J.Phys. (London) G1, 558 (1975)

R.P.Singhal, S.W.Brain, C.S.Curran, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight

Inelastic Scattering of Electrons from 90Zr

NUCLEAR REACTIONS 90Zr(e, e'), E=53.75-112.2 MeV; measured σ(E, e', θ). 90Zr deduced levels, J, π, B(λ).

doi: 10.1088/0305-4616/1/5/008
Citations: PlumX Metrics


1974LE17      J.Phys.(London) A7, 936 (1974)

E.W.Lees, A.Johnston, S.W.Brain, C.S.Curran, W.A.Gillespie, R.P.Singhal

The Study of the Excited States of 26Mg below 11 MeV by Inelastic Electron Scattering

NUCLEAR REACTIONS 26Mg(e, e'), E=56.89, 81.36, 82.75, 84.16, 85.09, 91.28, 95.74, 110.45, 110.71 MeV; measured σ(E, Ee', θ). 26Mg deduced levels, J, π, form factors β, B(λ), transition radii.

doi: 10.1088/0305-4470/7/8/005
Citations: PlumX Metrics


1974SI01      Nucl.Phys. A218, 189 (1974)

R.P.Singhal, S.W.Brain, W.A.Gillespie, A.Johnston, E.W.Lees, A.G.Slight

The B(E2) and R(tr) of 2+1 States in 90Zr and 60Ni

NUCLEAR REACTIONS 60Ni, 90Zr(e, e')E=45-250 MeV; measured σ. 60Ni, 90Zr levels deduced B(E2), transition radius.

doi: 10.1016/0375-9474(74)90030-X
Citations: PlumX Metrics


1973LE17      J.Phys.(London) A6, L116 (1973)

E.W.Lees, A.Johnston, S.W.Brain, C.S.Curran, W.A.Gillespie, R.P.Singhal

The B(E2) Value of the First Excited State of 26Mg

NUCLEAR REACTIONS 26Mg(e, e'); measured σ(θ). 26Mg level deduced B(E2).

doi: 10.1088/0305-4470/6/8/003
Citations: PlumX Metrics


1973SI39      Nucl.Phys. A216, 29 (1973)

R.P.Singhal, S.W.Brain, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, E.W.Lees

Elastic Scattering of Electrons from the N = 50 Isotones; 88Sr, 89Y, 90Zr and 92Mo

NUCLEAR REACTIONS 88Sr, 89Y, 90Zr, 92Mo(e, e), E0=25-120 MeV; measured σ(E). Deduced nuclear charge distributions.

doi: 10.1016/0375-9474(73)90515-0
Citations: PlumX Metrics


1972CU02      J.Phys.(London) A5, L39 (1972)

C.S.Curran, T.E.Drake, A.Johnston, S.W.Brain, W.A.Gillespie, E.W.Lees, R.P.Singhal, A.G.Slight

Nuclear Charge Distributions of the Isotopes 24Mg, 25Mg and 26Mg from Elastic Electron Scattering

NUCLEAR REACTIONS 24,25,26Mg(e, e), E =not given; measured σ(θ). 24,25,26Mg deduced nuclear charge distributions.

doi: 10.1088/0305-4470/5/4/001
Citations: PlumX Metrics


1971SI17      J.Phys.(London). A4, L93 (1971)

R.P.Singhal, C.S.Curran, T.E.Drake, W.A.Gillespie, A.Johnston, E.W.Lees

Nuclear Charge Distributions of 89Y, 90Zr and 92Mo by Elastic Electron Scattering

NUCLEAR REACTIONS 89Y, 90Zr, 92Mo(e, e), E not given; measured σ(θ). 89Y, 90Zr, 92Mo deduced nuclear charge distributions.


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