Nuclear Science References (NSR)

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NSR database version of April 26, 2024.

Search: Author = A.Johnston

Found 55 matches.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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 ^{160,161,162,164}Dy(¹⁶O, xnγ), E=70-110 MeV; measured Eγ, Iγ, γγ(t), γ(θ), I(ce). ^172,174,176W deduced levels, J, π, ICC, T_1/2.

doi: 10.1088/0305-4616/4/5/008
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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, T_1/2. Ge(Li), Ge, NE213 detectors. Enriched targets. Single-quasiparticle Coriolis mixing calculation.

doi: 10.1088/0305-4616/4/10/014
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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
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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
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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
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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
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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
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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, T_1/2. Ge, Ge(Li) detectors, enriched target.

doi: 10.1016/0375-9474(77)90109-9
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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
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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
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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
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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
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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 ^{160,161,162,162,163,164}Dy(¹⁶O, 4nγ), E=74-91 MeV; measured nγ(t), γγ(t), σ(E, Eγ, θ). ^{172,174,175,176}W deduced levels, K, J, π.

doi: 10.1088/0305-4616/2/12/001
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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
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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
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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
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1974JO16 Med.Phys. 1, 280 (1974)

A.S.Johnston

Photon Yield of 148.9-keV Gamma of ¹²³Xe

RADIOACTIVITY ¹²³Xe; measured T_1/2, photon yield.

doi: 10.1118/1.1637309
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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.

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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

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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

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