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NSR database version of April 27, 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 ^{110,112,114,116}Cd

NUCLEAR STRUCTURE ^{110,112,114,116}Cd; 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 ^{110,112,114,116}Cd(e, e'), E=68, 112 MeV; measured σ(θ). ^{110,112,114,116}Cd 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.