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NSR database version of April 11, 2024.

Search: Author = A.Johnston

Found 55 matches.

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2022BR05      Phys.Rev.Lett. 128, 212503 (2022)

L.J.Broussard, J.L.Barrow, L.DeBeer-Schmitt, T.Dennis, M.R.Fitzsimmons, M.J.Frost, C.E.Gilbert, F.M.Gonzalez, L.Heilbronn, E.B.Iverson, A.Johnston, Y.Kamyshkov, M.Kline, P.Lewiz, C.Matteson, J.Ternullo, L.Varriano, S.Vavra

Experimental Search for Neutron to Mirror Neutron Oscillations as an Explanation of the Neutron Lifetime Anomaly

NUCLEAR REACTIONS B, C(n, X), E cold; measured reaction products, En, In. 1NN; deduced neutron transmission, neutron conversions, increase the apparent neutron lifetime. The Spallation Neutron Source, the National Institute of Standards and Technology Beam Lifetime experiment.

doi: 10.1103/PhysRevLett.128.212503
Citations: PlumX Metrics


1992MA30      J.Phys.(London) G18, 1195 (1992)

I.J.D.MacGregor, A.Johnston, J.S.Ewing

Study of the M1 Isovector Strength in 28Si

NUCLEAR REACTIONS 28Si(e, e'), E=59-150 MeV; measured σ(E, θ). 28Si levels deduced form factors. Natural target. Shell model calculations.

doi: 10.1088/0954-3899/18/7/009
Citations: PlumX Metrics


1984MA08      Nucl.Phys. A412, 1 (1984)

I.J.D.Macgregor, A.Johnston, J.S.Ewing

Electron Scattering Measurements of Inelastic M3 Transitions

NUCLEAR REACTIONS 24Mg, 28Si(e, e'), E=82-160 MeV; measured σ(E, θ). 24Mg, 28Si levels deduced form factors. Enriched, natural targets. Shell model calculations.

doi: 10.1016/0375-9474(84)90382-8
Citations: PlumX Metrics


1980EN02      J.Phys.(London) G6, 1553 (1980)

J.B.A.England, T.R.Ophel, A.Johnston, A.F.Zeller

The 54Fe(d, t)53Fe Reaction and the Neutron Configuration in 54Fe

NUCLEAR REACTIONS 54Fe(d, t), E=18 MeV; measured σ(Et, θt). 53Fe deduced levels, S. DWBA analysis.

doi: 10.1088/0305-4616/6/12/010
Citations: PlumX Metrics


1980WA03      Phys.Rev. C21, 464 (1980)

P.M.Walker, G.D.Dracoulis, A.Johnston

Band Crossing in 172Hf

NUCLEAR REACTIONS 160Gd(16O, 4n), E=87 MeV; measured Eγ, γγ-coin, γγ(θ). 172Hf deduced levels. Band-crossing model.

doi: 10.1103/PhysRevC.21.464
Citations: PlumX Metrics


1980ZE02      Nucl.Phys. A344, 307 (1980)

A.F.Zeller, K.W.Kemper, T.R.Ophel, A.Johnston

Selective Population of Three-Particle States at High Excitation Energies in 15N

NUCLEAR REACTIONS 12C(7Li, α), E=48 MeV; measured σ(Eα). 15N deduced levels, J, π, Γ, configuration.

doi: 10.1016/0375-9474(80)90680-6
Citations: PlumX Metrics


1979CL10      Aust.J.Phys. 32, 283 (1979)

P.D.Clark, A.Johnston, T.R.Ophel

Widths of the 14.32 and 14.40 MeV Levels in 16O

NUCLEAR REACTIONS 14N(α, d), E=30 MeV; measured σ(Ed). 16O levels deduced Γ.

doi: 10.1071/PH790283
Citations: PlumX Metrics


1979KE05      Nucl.Phys. A320, 413 (1979)

K.W.Kemper, A.F.Zeller, T.R.Ophel, D.F.Hebbard, A.Johnston, D.C.Weisser

Elastic and Inelastic Scattering of 6Li and 7Li and 54Fe at E = 36-50 MeV

NUCLEAR REACTIONS 54Fe(6Li, 6Li), (6Li, 6Li'), E=38, 44, 50 MeV; 54Fe(7Li, 7Li), (7Li, 7Li'), E=36, 42, 48 MeV; measured σ(θ). 54Fe levels deduced optical-model parameters, deformation lengths.

doi: 10.1016/0375-9474(79)90198-2
Citations: PlumX Metrics


1979LE01      Phys.Rev.Lett. 42, 153 (1979)

J.R.Leigh, R.M.Diamond, A.Johnston, J.O.Newton, S.H.Sie

Fission Following Transfer to 232Th at Energies below the Coulomb Barrier

NUCLEAR REACTIONS 232Th(16O, X), E=75-95 MeV; 232Th(19F, X), E=85-95 MeV; measured σ(θ) for transfer-induced fission at sub-Coulomb energies.

doi: 10.1103/PhysRevLett.42.153
Citations: PlumX Metrics


1979ZE01      Nucl.Phys. A323, 477 (1979)

A.F.Zeller, K.W.Kemper, D.C.Weisser, T.R.Ophel, D.F.Hebbard, A.Johnston

Lithium-Induced Reactions on Carbon at 48 MeV

NUCLEAR REACTIONS 12C(7Li, 7Li), (7Li, 7Li'), (7Li, 6He), (7Li, 6Li), E=48; 13C(6Li, 6Li), (6Li, 6He), E=40 MeV; measured σ(θ); deduced optical-model parameters. 13N, 13C deduced S. Enriched targets, finite range DWBA analysis.

doi: 10.1016/0375-9474(79)90121-0
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


1978DR04      J.Phys.(London) G4, 713 (1978)

G.D.Dracoulis, P.M.Walker, A.Johnston

High-Spin States in 172W, 174W and 176W Studied by (16O, xn) Reactions: Decoupled Quasiparticle Bands and Backbending

NUCLEAR REACTIONS 160,161,162,164Dy(16O, xnγ), E=70-110 MeV; measured Eγ, Iγ, γγ(t), γ(θ), I(ce). 172,174,176W deduced levels, J, π, ICC, T1/2.

doi: 10.1088/0305-4616/4/5/008
Citations: PlumX Metrics


1978WA16      J.Phys.(London) G4, 1655 (1978)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh, M.G.Slocombe, I.F.Wright

High-Spin States and Single-Particle Structure in 173W and 175W

NUCLEAR REACTIONS 161,163Dy(16O, 4nγ), E=83-89 MeV; measured Eγ, Iγ, γγ-coin, nγ-coin, γ(θ). 173,175W deduced levels, J, π, T1/2. Ge(Li), Ge, NE213 detectors. Enriched targets. Single-quasiparticle Coriolis mixing calculation.

doi: 10.1088/0305-4616/4/10/014
Citations: PlumX Metrics


1978ZE05      Nucl.Phys. A309, 255 (1978)

A.F.Zeller, K.W.Kemper, T.R.Ophel, D.C.Weisser, D.F.Hebbard, A.Johnston, G.T.Hickey

The 118Sn(7Li, 6He)119Sb Reaction at 48 MeV

NUCLEAR REACTIONS 118Sn(6Li, 6Li), E=42 MeV; 118Sn(7Li, 7Li), 118Sn(7Li, 6He), E=48 MeV; measured σ(θ). 119Sb levels deduced S. Finite-range DWBA analysis; deduced optical model parameters. Enriched targets.

doi: 10.1016/0375-9474(78)90546-8
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


1977WA16      Nucl.Phys. A293, 481 (1977)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh

High-Spin States and Two-Quasiparticle Structure in 172Hf

NUCLEAR REACTIONS 160Gd(16O, 4n), E=75-84 MeV; measured Eγ, Iγ, γγ-coin, γγ(t), γ(θ). 172Hf deduced levels, K, J, π, T1/2. Ge, Ge(Li) detectors, enriched target.

doi: 10.1016/0375-9474(77)90109-9
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


1976WA16      J.Phys.(London) G2, L197 (1976)

P.M.Walker, G.D.Dracoulis, A.Johnston, J.R.Leigh, M.G.Slocombe, I.F.Wright

High Spin States and Backbending in the Light Tungsten Isotopes

NUCLEAR REACTIONS 160,161,162,162,163,164Dy(16O, 4nγ), E=74-91 MeV; measured nγ(t), γγ(t), σ(E, Eγ, θ). 172,174,175,176W deduced levels, K, J, π.

doi: 10.1088/0305-4616/2/12/001
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


1974JO10      J.Phys.(London) A7, 898 (1974)

A.Johnston, T.E.Drake

A Study of 24Mg by Inelastic Electron Scattering

NUCLEAR REACTIONS 24Mg(e, e'), E=64.94, 70.92, 72.6, 73.81, 81.66, 91.50, 99.21, 110.07, 110.82, 115.67 MeV; measured σ(E, Ee', θ). 24Mg deduced levels, J, π, form factors, 0-width, B(λ).

doi: 10.1088/0305-4470/7/8/004
Citations: PlumX Metrics


1974JO16      Med.Phys. 1, 280 (1974)

A.S.Johnston

Photon Yield of 148.9-keV Gamma of 123Xe

RADIOACTIVITY 123Xe; measured T1/2, photon yield.

doi: 10.1118/1.1637309
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.


1971SQ01      Nucl.Phys. A160, 602 (1971)

G.T.A.Squier, A.R.Johnston, E.W.Spiers, S.A.Harbison, N.M.Stewart

Cross-Section Measurements for the Reaction 10B(p, 3He)8Be

NUCLEAR REACTIONS 10B(p, 3He), E=49.5 MeV; measured σ(E(3He), θ). Enriched target.

doi: 10.1016/0375-9474(71)90100-X
Citations: PlumX Metrics


1971SQ02      Nucl.Phys. A167, 465 (1971)

G.T.A.Squier, A.R.Johnston, J.H.P.C.Megaw, R.J.Griffiths, F.G.Kingston

Asymmetry Measurements for the Reaction 10B(p, d)9B Induced by Polarized Protons

NUCLEAR REACTIONS 10B(polarized p, d), E=49.56 MeV; measured asymmetry(θ).

doi: 10.1016/0375-9474(71)90057-1
Citations: PlumX Metrics


1970HA25      Nucl.Phys. A150, 570 (1970)

S.A.Harbison, R.J.Griffiths, N.M.Stewart, A.R.Johnston, G.T.A.Squier

An Analysis of Polarization and Cross-Section Data for the p-3He System at 30 and 50 MeV

NUCLEAR REACTIONS 3He(p, p), E=50 MeV; measured P(θ); E=30, 50 MeV; measured σ(θ); deduced phase shifts. Enriched gas target.

doi: 10.1016/0375-9474(70)90418-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1197.


1970HA36      Nucl.Phys. A152, 503 (1970)

S.A.Harbison, R.J.Griffiths, N.M.Stewart, A.R.Johnston, G.T.A.Squier

An Analysis of the Angular Distributions of the Reactions 4He(p, d)3He, 4He(p, t)2p, 4He(p, 3He)pn and 3He(p, d)2p

NUCLEAR REACTIONS 4He(p, d), E=49.5 MeV; measured σ(θ). 4He(p, t), (p, 3He), 3He(p, d), E=49.5 MeV; 3He(p, d), E=30.5 MeV; analysed σ(θ).

doi: 10.1016/0375-9474(70)90928-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0528.


1970SQ01      Nucl.Phys. A141, 158 (1970)

G.T.A.Squier, A.R.Johnston, E.W.Spiers, S.A.Harbison, N.M.Stewart

Cross-Section Measurements for the Reactions 10B(p, d)9B and 10B(p, t)8B

NUCLEAR REACTIONS 10B(p, d), (p, t), (p, p), E=49.5 MeV; measured σ(Ed, θ), σ(Et, θ). 8,9B deduced levels, J. Enriched target.

doi: 10.1016/0375-9474(70)90301-5
Citations: PlumX Metrics


1969HA16      Nucl.Phys. A130, 513 (1969)

S.A.Harbison, R.J.Griffiths, F.G.Kingston, A.R.Johnston, G.T.A.Squier

Nucleon-Nucleon Final-State Interactions in the Reactions 3He(p, d)2p, 4He(p, t)2p and 4He(p, 3He)pn

NUCLEAR REACTIONS 3He(p, d), Ep=30, 50 MeV; 4He(p, t), (p, 3He), Ep=50 MeV; measured energy spectra, σ(Ed, Et, E(3He), θ). Enriched gas target.

doi: 10.1016/0375-9474(69)90863-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0474.


1969KI03      Nucl.Phys. A124, 225(1969)

F.G.Kingston, R.J.Griffiths, A.R.Johnston, W.R.Gibson, E.A.McClatchie, J.H.P.C.Megaw

A Study of the 26Mg(p, t)24Mg and 26Mg(p, 3He)24Na Reactions at 50 MeV

NUCLEAR REACTIONS 26Mg(p, t), 26Mg(p, 3He), E=50 MeV; measured σ(E(3He), θ), σ(Et, θ). 24Mg, 24Na deduced levels, T. Enriched target.

doi: 10.1016/0375-9474(69)90531-4
Citations: PlumX Metrics


1968HA04      Nucl. Phys. A108, 478(1968)

S.A.Harbison, F.G.Kingston, A.R.Johnston, E.A.McClatchie

A Search for Excited States in 3He by the 3He(p, p)3He* Reaction

NUCLEAR REACTIONS 3He(p, p'), E = 30 MeV; measured σ(Ep', θ); deduced no levels. Enriched target.

doi: 10.1016/0375-9474(68)90103-6
Citations: PlumX Metrics


1968HA12      Nucl.Phys. A112, 137(1968)

S.A.Harbison, F.G.Kingston, R.J.Griffiths, A.R.Johnston, J.H.P.C.Megaw

Polarization in the Elastic Scattering of 30 MeV Protons by 3He

NUCLEAR REACTIONS 3He(p, p), E=30 MeV; measured polarization P(θ).

doi: 10.1016/0375-9474(68)90224-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1197.


1968ME22      Nucl.Phys. A122, 689(1968)

J.H.P.C.Megaw, A.R.Johnston, W.R.Gibson, F.G.Kingston

Polarization in the Elastic Scattering of 9.5 MeV and 21.6 MeV Protons By Deuterons

NUCLEAR REACTIONS 2H(p, p)2H, E=9.5, 21.6 MeV; measured P(θ). Enriched target.

doi: 10.1016/0375-9474(68)90589-7
Citations: PlumX Metrics


1968SQ01      Nucl.Phys. A119, 369 (1968)

G.T.A.Squier, E.A.McClatchie, A.R.Johnston, R.J.Batten, J.B.A.England, F.G.Kingston

Elastic and Inelastic Scattering of 3He Particles from 10B at 32 MeV

NUCLEAR REACTIONS 10B(3He, 3He'), E=32.46 MeV; measured σ(θ, E(3He)'). 10B levels deduced distortion parameters β(L). Enriched target.

doi: 10.1016/0375-9474(68)90307-2
Citations: PlumX Metrics


1967JO05      Priv.Comm. (1967)

A.S.Johnston, G.M.Julian

NUCLEAR STRUCTURE 106Rh; measured not abstracted; deduced nuclear properties.


1967JU04      Phys.Rev. 163, 1323 (1967)

G.M.Julian, S.Jha, A.S.Johnston

Excited States of 128Xe

NUCLEAR STRUCTURE 128I, 128Cs, 128Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.163.1323
Citations: PlumX Metrics


1966JO01      Phys.Letters 21, 309 (1966)

A.R.Johnston, W.R.Gibson, E.A.McClatchie, J.H.P.C.Megaw, R.J.Griffiths

Polarization in the Elastic Scattering of 50 MeV Protons by Deuterons at Backward Angles

NUCLEAR STRUCTURE 1H; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90829-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1742.


1966KI07      Phys.Letters 22, 458 (1966)

F.G.Kingston, R.J.Griffiths, A.R.Johnston, W.R.Gibson, E.A.McClatchie

The T = 2 Isobaric Multiplet at Mass 24

NUCLEAR STRUCTURE 24Na, 24Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)91226-1
Citations: PlumX Metrics


1965JO14      Phys.Letters 19, 289 (1965)

A.R.Johnston, W.R.Gibson, J.H.P.C.Megaw, R.J.Griffiths, R.M.Eisberg

Polarization in the Elastic Scattering at Backward Angles of 30 MeV Protons from Deuterons

NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90991-1
Citations: PlumX Metrics


1964JH01      Bull.Am.Phys.Soc. 9, No.4, 472, HA15 (1964)

S.Jha, T.D.Nainan, A.S.Johnston, K.R.Reddy, G.V.S.Rayudu

On the Decay of 1.25-min 82Rb

NUCLEAR STRUCTURE 82Rb; measured not abstracted; deduced nuclear properties.


1964JO07      Bull.Am.Phys.Soc. 9, No.4, 485, JA14 (1964)

A.S.Johnston, S.Jha, J.L.Power, R.Leonard

On the Excited States of 130Xe

NUCLEAR STRUCTURE 130Cs; measured not abstracted; deduced nuclear properties.


1964NA01      Bull.Am.Phys.Soc. 9, No.1, 17, BB5 (1964)

T.D.Nainan, A.S.Johnston, S.Jha

On the Decay of 66-min In110

NUCLEAR STRUCTURE 110In; measured not abstracted; deduced nuclear properties.


1964NA03      Phys.Rev. 135, B601 (1964)

T.D.Nainan, A.S.Johnston, S.Jha

Decay of 66-min In110

NUCLEAR STRUCTURE 110In; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.135.B601
Citations: PlumX Metrics


1964RE02      Bull.Am.Phys.Soc. 9, No.1, 17, BB2 (1964)

K.R.Reddy, A.S.Johnston, S.Jha

On the Decay of 32.9-h Sr83

NUCLEAR STRUCTURE 83Sr; measured not abstracted; deduced nuclear properties.


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Note: The following list of authors and aliases matches the search parameter A.Johnston: , A.R.JOHNSTON, A.S.JOHNSTON