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Search: Author = R.D.Lawson

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1992CH05      Phys.Rev. C45, 1260 (1992)

S.Chiba, P.T.Guenther, A.B.Smith, M.Sugimoto, R.D.Lawson

Fast-Neutron Interaction with Elemental Zirconium, and the Dispersive Optical Model

NUCLEAR REACTIONS Zr(n, n), (n, n'), E ≈ 1.5-10 MeV; measured σ(θ); deduced σ(E), model parameters. Optical-statistical models.

doi: 10.1103/PhysRevC.45.1260
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13505.

1990CH40      Phys.Rev. C42, 2487 (1990)

S.Chiba, P.T.Guenther, R.D.Lawson, A.B.Smith

Neutron Scattering from Elemental Indium: Optical model and bound-state potential

NUCLEAR REACTIONS In(n, n), E=4.5-10 MeV; calculated σ(θ); deduced optical potential parameters. Other data input.

doi: 10.1103/PhysRevC.42.2487
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13193.

1990LA24      Nucl.Phys. A519, 487 (1990)

R.D.Lawson, P.T.Guenther, A.B.Smith

Ambiguities in the Elastic Scattering of 8 MeV Neutrons from Adjacent Nuclei

NUCLEAR REACTIONS 51V, Cr, 59Co, 58Ni, Cu, Zn, 89Y, 93Nb, Zr, In, Cd, 209Bi, Pb(n, n), E=8 MeV; measured σ(θ), ratio for adjacent nuclei; deduced ambiguities. Optical model.

doi: 10.1016/0375-9474(90)90442-O
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13188.

1989BR22      Z.Phys. A334, 11 (1989)

R.Broda, P.J.Daly, J.H.McNeill, Z.W.Grabowski, R.V.F.Janssens, R.D.Lawson, D.C.Radford

Decays of Millisecond Isomers in Odd-Odd N = 81 Nuclei 146Tb, 148Ho and 150Tm

NUCLEAR REACTIONS 90Zr, 92Mo, 89Y(60Ni, n2p), E=245 MeV; measured Eγ, Iγ, γγ-coin.

RADIOACTIVITY 146Tb [from 89Y(60Ni, n2p), E=245 MeV]; 148Ho [from 90Zr(60Ni, np), E=245 MeV]; 150Tm [from 92Mo(60Ni, np), E=245 MeV]; measured Eγ, Iγ, γγ-coin; deduced isomer T1/2, decay features, Iγ, γ-multipolarity, B(λ), configuration.

1989LA09      Nucl.Phys. A493, 267 (1989)

R.D.Lawson, P.T.Guenther, A.B.Smith

Neutron Scattering and the Fermi Surface Anomaly in 51V

NUCLEAR REACTIONS 51V(n, n), (n, n'), E=4.5-10 MeV; measured σ(θ) versus E. Optical model interpretation.

doi: 10.1016/0375-9474(89)90398-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13135.

1989SE01      Phys.Rev. C39, 749 (1989)

R.E.Segel, A.Amusa, D.F.Geesaman, R.D.Lawson, B.Zeidman, C.Olmer, A.D.Bacher, G.T.Emery, C.W.Glover, H.Nann, W.P.Jones, S.Y.van der Werf, R.A.Lindgren

Fragmentation of High-Spin Particle-Hole States in 26Mg

NUCLEAR REACTIONS 26Mg(polarized p, p'), E=135 MeV; measured σ(θ), A(θ). 26Mg deduced levels, J, π. 28Si deduced levels, J, π, isoscalar, isovector excitation amplitudes. Other data input.

doi: 10.1103/PhysRevC.39.749
Citations: PlumX Metrics

1988SM02      Nucl.Phys. A483, 50 (1988)

A.B.Smith, P.T.Guenther, R.D.Lawson

Energy Dependence of the Optical Model Potential for Fast Neutron Scattering from Cobalt

NUCLEAR REACTIONS 59Co(n, n), (n, n'), E=1.5-10 MeV; measured σ(θ) vs E. Optical coupled-channels models.

doi: 10.1016/0375-9474(88)90064-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13131.

1988SO07      Phys.Rev. C38, 654 (1988)

D.I.Sober, L.W.Fagg, B.Zeidman, R.D.Lawson, D.F.Geesaman, G.C.Morrison, O.Karban, X.K.Maruyama, H.de Vries, E.A.J.M.Offermann, C.W.de Jager, R.A.Lindgren, J.F.A.van Hienen

Electroexcitation of 8- States in 52Cr

NUCLEAR REACTIONS 52Cr(e, e'), E=170-260 MeV; measured σ(E(e')), θ=115°, 154°. 52Cr deduced B(M8), total T=2, T=3 strengths, sums for M8 transitions. Shell model.

doi: 10.1103/PhysRevC.38.654
Citations: PlumX Metrics

1987LA21      Phys.Rev. C36, 1298 (1987)

R.D.Lawson, P.T.Guenther, A.B.Smith

Energy Dependence of the Optical-Model Potential for Fast-Neutron Scattering from Bismuth

NUCLEAR REACTIONS 209Bi(n, n), E=4.5-10 MeV; measured σ(θ); deduced σ(E), potential energy dependence. Optical model, other data input.

doi: 10.1103/PhysRevC.36.1298
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13120.

1987ME21      Ann.Nucl.Energy 14, 603 (1987)

J.W.Meadows, D.L.Smith, R.D.Lawson

Differential Measurements and an Evaluation of the 59Co(n, α)56Mn Reaction Cross-Section

NUCLEAR REACTIONS 59Co(n, α), E=5.07-9.98 MeV; measured σ(θ); compiled σ(E). Activation method. Model calculations.

doi: 10.1016/0306-4549(87)90095-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13113.

1986LA30      Phys.Rev. C34, 1599 (1986)

R.D.Lawson, P.T.Guenther, A.B.Smith

Search for the Fermi-Surface Anomaly in Fast-Neutron Scattering from Yttrium

NUCLEAR REACTIONS 89Y(n, n), E=4-10 MeV; measured σ(θ, En); calculated σ(E); deduced no Fermi surface anomaly. Optical, statistical model analyses.

doi: 10.1103/PhysRevC.34.1599
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12979.

1986MC14      Z.Phys. A325, 27 (1986)

J.McNeill, R.Broda, Y.H.Chung, P.J.Daly, Z.W.Grabowski, H.Helppi, M.Kortelahti, R.V.F.Janssens, T.L.Khoo, R.D.Lawson, D.C.Radford, J.Blomqvist

Level Structure of Proton-Rich N = 83 Nuclei 150Ho and 152Tm

NUCLEAR REACTIONS 92Zr, 94Mo(60Ni, np), 93Nb(60Ni, n2p), E=240-250 MeV; measured γγ-coin, sum spectra, γ(t). 150Ho, 152Tm deduced levels, J, π, isomer, T1/2, decay characteristics, B(λ), γ-branching, γ-multipolarity, ICC. Enriched metallic targets, NaI sum spectrometer, Ge(Li) detectors. Shell model calculations.

1986SM03      Nucl.Phys. A455, 344 (1986)

A.B.Smith, P.T.Guenther, R.D.Lawson

On the Energy Dependence of the Optical Model of Neutron Scattering from Niobium

NUCLEAR REACTIONS 93Nb(n, n), E=1.5-10 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1016/0375-9474(86)90022-9
Citations: PlumX Metrics

1985BR07      Z.Phys. A321, 287 (1985)

R.Broda, P.J.Daly, Z.W.Grabowski, H.Helppi, M.Kortelahti, J.McNeill, R.V.F.Janssens, R.D.Lawson, D.C.Radford, J.Blomqvist

Two-Proton Neutron-Hole Yrast Excitations in 14766Dy81

NUCLEAR REACTIONS 89Y(60Ni, np), 90Zr(60Ni, n2p), 92Zr(58Ni, n2p), E=230-250 MeV; measured Eγ, Iγ, γγ-coin. 147Dy deduced levels, J, π, yrast sequence, γ-multipolarity, branching, transition widths, ICC, seniority characteristics, B(λ), configurations.

doi: 10.1007/BF01493450
Citations: PlumX Metrics

1984GE06      Phys.Rev. C30, 952 (1984)

D.F.Geesaman, R.D.Lawson, B.Zeidman, G.C.Morrison, A.D.Bacher, C.Olmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, R.L.Boudrie, C.L.Morris, R.A.Lindgren, W.H.Kelly, R.E.Segel, L.W.Swenson

Quenching of Isoscalar Spin-Flip Strength in 54Fe

NUCLEAR REACTIONS 54Fe(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 54Fe levels deduced isoscalar, isovector strengths.

doi: 10.1103/PhysRevC.30.952
Citations: PlumX Metrics

1984KU07      Phys.Rev. C29, 2303 (1984)

D.Kurath, R.D.Lawson

Effect of Delta Admixture on 1p-Shell M1 Matrix Elements

NUCLEAR STRUCTURE 11,12,13B, 12,13,14C, 14,15N; calculated M1 matrix elements; deduced isobar resonance role.

doi: 10.1103/PhysRevC.29.2303
Citations: PlumX Metrics

1983AM02      Phys.Rev.Lett. 51, 103 (1983)

A.Amusa, R.D.Lawson

Quenching of Stretched Magnetic Transitions

NUCLEAR STRUCTURE 28Si; calculated yrast states, B(M1), nucleon transfer reaction strengths, M6 transition strength quenching. Enlarged shell model space, effective interactions.

doi: 10.1103/PhysRevLett.51.103
Citations: PlumX Metrics

1983AM06      Z.Phys. A314, 205 (1983)

A.Amusa, R.D.Lawson

High Spin States in 91Tc

NUCLEAR STRUCTURE 91Tc; calculated levels, yrast sequence, B(λ). Shell model.

doi: 10.1007/BF01879879
Citations: PlumX Metrics

1983LA13      Phys.Lett. 125B, 255 (1983)


The Effect of the Δ(1236) on the g-Factor of Nucleons

NUCLEAR STRUCTURE A=16, 40, 90, 208; calculated orbital nucleon g, central, tensor parts. 48Ca; calculated B(M1). First order perturbation theory, isobar effects.

doi: 10.1016/0370-2693(83)91279-0
Citations: PlumX Metrics

1982AM04      Z.Phys. A307, 333 (1982)

A.Amusa, R.D.Lawson

High Spin States in 94Ru and 95Rh

NUCLEAR STRUCTURE 94Ru, 95Rh; calculated levels, B(λ), γ-branching ratio. Shell model.

doi: 10.1007/BF01421295
Citations: PlumX Metrics

1982HE08      Phys.Lett. 115B, 11 (1982)

H.Helppi, Y.H.Chung, P.J.Daly, S.R.Faber, A.Pakkanen, I.Ahmad, P.Chowdhury, Z.W.Grabowski, T.L.Khoo, R.D.Lawson, J.Blomqvist

Yrast (πh11/2)(n) Excitations in Proton-Rich N = 82 Nuclei

NUCLEAR REACTIONS 92,94Zr, 93Nb, 92,94,95Mo(58Ni, X), (62Ni, X), E=225-285 MeV; measured σ(Eγ), γγ-, γ(X-ray)-coin. 150Er, 151Tm deduced levels, γ-branching, J, π, isomer T1/2, B(λ), configuration.

doi: 10.1016/0370-2693(82)90504-4
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1982MA30      Phys.Rev. C26, 500 (1982)

W.Mayer, D.Pereira, K.E.Rehm, H.J.Scheerer, H.J.Korner, G.Korschinek, W.Mayer, P.Sperr, S.C.Pieper, R.D.Lawson

Strong Population of Excited 0+ States in Even Zr Isotopes Observed with the (14C, 16O) Reaction

NUCLEAR REACTIONS 92,100Mo(14C, 14C), (14C, 14C'), (14C, 16O), 94,96,98Mo(14C, 16O), E=71 MeV; measured σ(θ), σ(E(16O)); deduced optical model parameters. 90,92,94,96,98Zr levels deduced spectroscopic amplitudes. DWBA analysis.

doi: 10.1103/PhysRevC.26.500
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1567.

1981LA26      Z.Phys. A303, 51 (1981)


(πh11/2(n)) States Expected in 15068Er82, 15169Tm82 and 15270Yb82

NUCLEAR STRUCTURE 150Er, 151Tm, 152Yb; calculated levels, B(E2). Shell model.

doi: 10.1007/BF01420010
Citations: PlumX Metrics

1981LI05      Phys.Rev.Lett. 46, 706 (1981)

R.A.Lindgren, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson, R.D.Lawson, W.Teeters, C.F.Williamson, S.Kowalski, X.K.Maruyama

Comparison of Inelastic Electron Scattering with [g9/2 x (f1/2-3)(J)] (8)- Shell-Model Calculations for the T=1 and T=2, 8-States in 54Fe

NUCLEAR REACTIONS 54Fe(e, e'), E=205.1 MeV; measured σ(E(e')), form factors. 54Fe levels deduced J, π, T, γ-multipolarity, B(M8) strength distribution. Shell model calculations.

doi: 10.1103/PhysRevLett.46.706
Citations: PlumX Metrics

1981WI08      Phys.Lett. 103B, 413 (1981)

J.Wilson, Y.H.Chung, S.R.Faber, A.Pakkanen, P.J.Daly, I.Ahmad, P.Chowdhury, T.L.Khoo, R.D.Lawson, R.K.Smither

Shell Model Yrast States of the N = 83 Nucleus 150Ho

NUCLEAR REACTIONS 122Te(32S, 3np), 121Sb(32S, 3n), E=155-180 MeV; measured γγ-coin, γγ(t), γ(t). 150Ho deduced levels, J, π, T1/2, yrast sequence, γ-branching, B(E2), configuration. Shell model interpretation.

doi: 10.1016/0370-2693(81)90072-1
Citations: PlumX Metrics

1980LE04      Phys.Rev. C21, 679 (1980)

T.-S.H.Lee, R.D.Lawson

Inelastic Pion Scattering from 18O

NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E ≈ 164 MeV; calculated σ(θ). DWIA, relativistic non-local effects, shell model.

doi: 10.1103/PhysRevC.21.679
Citations: PlumX Metrics

1980WI11      Z.Phys. A296, 185 (1980)

J.Wilson, S.R.Faber, P.J.Daly, I.Ahmad, J.Borggreen, P.Chowdhury, T.L.Khoo, R.D.Lawson, R.K.Smither, J.Blomqvist

The πh311/2 Spectrum in the Three Valence Proton Nucleus 14967Ho82

NUCLEAR REACTIONS 121Sb, 122Te(32S, xnyp), E=155-180 MeV; measured Eγ, Iγ, γγ-coin, γγ(t). 149Ho deduced levels, T1/2, J, π, γ-multipolarity, configuration. Enriched targets.

doi: 10.1007/BF01412660
Citations: PlumX Metrics

1979FO14      Phys.Rev. C20, 1228 (1979)

H.T.Fortune, G.E.Moore, L.Bland, M.E.Cobern, S.Mordechai, R.Middleton, R.D.Lawson

Reaction 15N(t, p)17N

NUCLEAR REACTIONS 15N(t, p), E=15.0 MeV; measured σ(Ep, θ). 17N levels deduced L, π, J. Enriched gas target. Comparison with shell model.

doi: 10.1103/PhysRevC.20.1228
Citations: PlumX Metrics

1979LA06      Phys.Rev. C19, 2359 (1979)


Nuclear Charge Dependent Interactions in the 1p Shell

NUCLEAR STRUCTURE A=8-14; calculated isotensor coefficient in mass-multiplet relationship; deduced need for isotensor nucleon-nucleon interaction. Shell model.

doi: 10.1103/PhysRevC.19.2359
Citations: PlumX Metrics

1979LA10      Phys.Rev. C20, 842 (1979)


Isospin Mixing in 19F

NUCLEAR STRUCTURE 19F; calculated isospin mixing for T=1/2 yrast level. Shell model, isoscalar nucleon-nucleon interaction, experimental single-particle spacing of A=17 nuclei.

doi: 10.1103/PhysRevC.20.842
Citations: PlumX Metrics

1977LA12      Phys.Rev. C16, 1609 (1977)

R.D.Lawson, A.Muller-Arnke

Properties of the d3/2-Hole States in the 1f7/2 Nuclei

NUCLEAR STRUCTURE 43,47Sc, 45Ti; calculated g. Shell model.

doi: 10.1103/PhysRevC.16.1609
Citations: PlumX Metrics

1976DI06      Phys.Rev. C13, 1745 (1976)

W.R.Dixon, R.S.Storey, J.J.Simpson, R.D.Lawson

Upper Limit on ΔT = 2, E2 Transition in 44Ti

NUCLEAR REACTIONS 40Ca(α, γ); measured γ-spectra. 44Ti deduced levels, B(E2).

doi: 10.1103/PhysRevC.13.1745
Citations: PlumX Metrics

1976GL05      Nucl.Phys. A262, 253 (1976)

D.H.Gloeckner, R.D.Lawson, F.J.D.Serduke

Allowed Beta Decay of the N = 49 Isotones

RADIOACTIVITY 89Zr, 90Nb, 91Mo, 92Tc, 93Ru; calculated log ft.

doi: 10.1016/0375-9474(76)90619-9
Citations: PlumX Metrics

1976LA13      Phys.Rev. C14, 1245 (1976)

R.D.Lawson, F.J.D.Serduke, H.T.Fortune

Structure of Low-Lying Positive-Parity States of 18O

NUCLEAR STRUCTURE 18O; calculated wave functions.

doi: 10.1103/PhysRevC.14.1245
Citations: PlumX Metrics

1976SE01      Nucl.Phys. A256, 45 (1976)

F.J.D.Serduke, R.D.Lawson, D.H.Gloeckner

Shell-Model Study of the N=49 Isotones

NUCLEAR STRUCTURE 88Y, 89Zr, 90Nb, 91Mo, 92Tc, 93Ru; calculated levels, T1/2. 88Y, 89Zr, 91Nb; calculated B(λ). Shell model.

doi: 10.1016/0375-9474(76)90094-4
Citations: PlumX Metrics

1975GL02      Phys.Rev. C11, 1832 (1975)

D.H.Gloeckner, R.D.Lawson

E6 Transition in 53Fe

NUCLEAR STRUCTURE 53Fe; calculated B(E6).

doi: 10.1103/PhysRevC.11.1832
Citations: PlumX Metrics

1975GL05      Phys.Lett. 56B, 301 (1975)

D.H.Gloeckner, R.D.Lawson

The Isospin Forbidden 1-→0+ Transition in 40Ca

NUCLEAR STRUCTURE 40Ca; calculated B(E1).

doi: 10.1016/0370-2693(75)90304-4
Citations: PlumX Metrics

1974GL04      Phys.Rev. C9, 2071 (1974)

D.H.Gloeckner, R.D.Lawson, F.J.D.Serduke

Neutron-Rich Argon Nuclei

NUCLEAR STRUCTURE 43Ar calculated levels, J; 43,44,45,46Ar calculated binding energies.

doi: 10.1103/PhysRevC.9.2071
Citations: PlumX Metrics

1974GL09      Phys.Lett. 53B, 313 (1974)

D.H.Gloeckner, R.D.Lawson

Spurious Center-of-Mass Motion

NUCLEAR STRUCTURE 16O; calculated levels.

doi: 10.1016/0370-2693(74)90390-6
Citations: PlumX Metrics

1973GL02      Phys.Rev. C7, 1913 (1973)

D.H.Gloeckner, R.D.Lawson, F.J.D.Serduke

Properties of the Argon Isotopes

NUCLEAR STRUCTURE 41,42,43,44,45,46,47,48,49,50Ca, 38Cl, 40K calculated levels. 39,40,41,42Ar calculated levels, γ-branching, T1/2.

doi: 10.1103/PhysRevC.7.1913
Citations: PlumX Metrics

1972GL02      Phys.Lett. 40B, 597 (1972)

D.H.Gloeckner, M.H.Macfarlane, R.D.Lawson, F.J.D.Serduke

Inhibited Transitions and Isomeric States in the N = 50 Isotones

NUCLEAR STRUCTURE 90Zr, 92Mo, 94Ru; calculated E2 T1/2, B(E2). Shell model.

doi: 10.1016/0370-2693(72)90604-1
Citations: PlumX Metrics

1972KU22      Phys.Rev. C6, 901 (1972)

D.Kurath, R.D.Lawson

Magnetic Multipole Properties of 38Cl and 40K

NUCLEAR STRUCTURE 38Cl, 40K; calculated levels, μ, configurations; analyzed effects of weak p-H admixtures.

doi: 10.1103/PhysRevC.6.901
Citations: PlumX Metrics

1971HO27      Ann.Phys.(N.Y.) 63, 607 (1971)

R.E.Holland, R.D.Lawson, F.J.Lynch

Electric-Quadrupole Isomers in 90Nb and 92Tc

RADIOACTIVITY 90mNb, 92mTc; measured T1/2 for E2 isomers.

doi: 10.1016/0003-4916(71)90033-9
Citations: PlumX Metrics

1971LA15      Nucl.Phys. A173, 17 (1971)


Anomalous E2 Matrix Elements

NUCLEAR STRUCTURE 36Cl, 48Ti, 42Sc; calculated quadrupole moment. 48Ti E2 transition calculated T1/2. 48V; calculated levels. 42,44,46,48Ca, 46,48Ti, 43,45,47,49Sc, 47,49V; calculated energy of core-excited 0+ state. 46V, 50Mn; calculated levels.

doi: 10.1016/0375-9474(71)90745-7
Citations: PlumX Metrics

1970LY02      Phys.Lett. 32B, 38 (1970)

F.J.Lynch, K.-E.Nysten, R.E.Holland, R.D.Lawson

Lifetimes of Low-Energy Levels in 45Ti

NUCLEAR REACTIONS 45Sc(p, nγ), E=6 MeV; 42Ca(α, nγ), E=10 MeV; measured pγ-, αγ-delay. 45Ti levels deduced T1/2.

doi: 10.1016/0370-2693(70)90330-8
Citations: PlumX Metrics

1969LA19      Nucl.Phys. A133, 473(1969)

R.D.Lawson, J.M.Soper

Shell-Model Matrix Elements from a Realistic Potential

NUCLEAR STRUCTURE 6He; calculated shell-model two-body matrix elements.

doi: 10.1016/0375-9474(69)90648-4
Citations: PlumX Metrics

1968AR02      Nucl.Phys. A108, 94 (1968)

A.Arima, S.Cohen, R.D.Lawson, M.H.Macfarlane

A Shell-Model Study of the Isotopes of O, F and Ne

doi: 10.1016/0375-9474(68)90147-4
Citations: PlumX Metrics

1967CO22      Phys.Rev. 160, 903 (1967)

S.Cohen, R.D.Lawson, M.H.Macfarlane, S.P.Pandya, M.Soga

Shell Model of the Nickel Isotopes

NUCLEAR STRUCTURE 66Ni, 64Ni, 62Ni, 61Ni, 65Ni, 63Ni, 59Ni, 58Ni, 60Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.903
Citations: PlumX Metrics

1966LA07      Phys.Rev.Letters 16, 1006 (1966)

R.D.Lawson, R.E.Segel

Parity Mixing in Hf180

NUCLEAR STRUCTURE 180Hf; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.16.1006
Citations: PlumX Metrics

1966LA12      Phys.Lett. 22, 68 (1966)

R.D.Lawson, M.H.MacFarlane, T.T.S.Kuo

The Reaction Matrix and Effective Shell-Model Interactions for the Ni Isotopes

NUCLEAR STRUCTURE 59Ni, 60Ni, 58Ni, 64Ni, 63Ni, 65Ni, 62Ni, 61Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90562-2
Citations: PlumX Metrics

1965ER04      Phys.Rev.Letters 14, 915 (1965)

J.R.Erskine, R.E.Holland, R.D.Lawson, M.H.Macfarlane, J.P.Schiffer

Proton-Core Excitation in the Ground State of O18

NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.15.915
Citations: PlumX Metrics

1965LA04      Phys.Rev.Letters 14, 152 (1965)

R.D.Lawson, M.H.Macfarlane

M2 Lifetimes and Core Excitation in the Scandium Isotopes

NUCLEAR STRUCTURE 43Sc, 47Sc, 45Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.14.152
Citations: PlumX Metrics

1964CO23      Bull. Am. Phys. Soc. 9, No. 6, 650, Q8 (1964)

S.Cohen, R.D.Lawson, M.H.Macfarlane, S.P.Pandya, M.Soga

Shell-Model Studies of the Isotopes of Ni

NUCLEAR STRUCTURE Ni; measured not abstracted; deduced nuclear properties.

1964CO24      Phys. Letters 9, 180 (1964)

S.Cohen, R.D.Lawson, M.H.Macfarlane, M.Soga

Effective Shell-Model Interaction for the Isotopes of Oxygen

NUCLEAR STRUCTURE 19O, 20O, 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90135-0
Citations: PlumX Metrics

1964LA15      Bull.Am.Phys.Soc. 9, No.6, 650, Q4 (1964)

R.D.Lawson, M.H.Macfarlane, M.Soga, S.Cohen

Metastable d3/2-Hole States in Sc45 and Sc47

NUCLEAR STRUCTURE Sc; measured not abstracted; deduced nuclear properties.

1962LA23      TID-15266 (1962); Nuclear Sci.Abstr. 17, 2953, Abstr.22565 (1963)


First Excited State in Mg26

NUCLEAR STRUCTURE 26Mg; measured not abstracted; deduced nuclear properties.

1961KU17      Nuclear Phys. 23, 5 (1961)

D.Kurath, R.D.Lawson

Positive-Parity States in Mass-13 Nuclei

doi: 10.1016/0029-5582(61)90234-6
Citations: PlumX Metrics

1960LA16      Phys.Rev. 117, 174 (1960)

R.D.Lawson, M.Goeppert-Mayer

Harmonic Oscillator Wave Functions in Nuclear Spectroscopy

doi: 10.1103/PhysRev.117.174
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