NSR Query Results
Output year order : Descending NSR database version of May 6, 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1974JO10 J.Phys.(London) A7, 898 (1974) 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
1974JO16 Med.Phys. 1, 280 (1974) Photon Yield of 148.9-keV Gamma of 123Xe RADIOACTIVITY 123Xe; measured T1/2, photon yield.
doi: 10.1118/1.1637309
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1967JO05 Priv.Comm. (1967) 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
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
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
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
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
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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