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Search: Author = H.C.Evans

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1996OU01      Phys.Rev. C54, 1982 (1996)

J.M.L.Ouellet, M.N.Butler, H.C.Evans, H.W.Lee, J.R.Leslie, J.D.MacArthur, W.McLatchie, H.-B.Mak, P.Skensved, J.L.Whitton, X.Zhao

12C(α, γ)16O Cross Sections at Stellar Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), E=1.5-3 MeV; measured σ(θ); deduced E1, E2 σ, astrophysical S-factor. K-matrix, R-matrix, cluster models.

doi: 10.1103/PhysRevC.54.1982
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0439.

1994IL01      Nucl.Phys. A571, 132 (1994)

C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, R.E.Azuma, G.Roters, H.P.Trautvetter, H.C.Evans

Explosive Hydrogen Burning of 35Cl

NUCLEAR REACTIONS 35Cl(3He, d), E=15 MeV; measured σ(θ), σ(Ed). 32S(6Li, d), E=32 MeV; measured σ(Ed). 32S(α, γ), E ≈ resonance; measured Eγ, Iγ. 35Cl(p, γ), E ≈ 200-800 keV; measured γ yield vs E , stellar rates. 35Cl(p, X), E=177 keV; measured particle spectra. 36Ar deduced levels, J, π, L, spectroscopic factors, γ-branching ratios, resonance strengths. Deduced no evidence for (p, α) reactions.

doi: 10.1016/0375-9474(94)90345-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0908.

1993IL01      Nucl.Phys. A559, 83 (1993)

C.Iliadis, J.Gorres, J.G.Ross, K.W.Scheller, M.Wiescher, C.Grama, Th.Schange, H.P.Trautvetter, H.C.Evans

Explosive Hydrogen Burning of 31P

NUCLEAR REACTIONS, ICPND 31P(p, γ), (p, α), E=160-370 keV; 28Si(α, γ), E=2.4-2.6 MeV; measured γ yield vs E; deduced stellar reaction rates, temperature dependence. 32S deduced proton thershold state features.

doi: 10.1016/0375-9474(93)90181-V
Citations: PlumX Metrics

1993KO38      Phys.Rev. C48, 2375 (1993)

R.J.Komar, H.-B.Mak, J.R.Leslie, H.C.Evans, E.Bonvin, E.D.Earle, T.K.Alexander

3He(n, γ)4He Cross Section and the Photodisintegration of 4He

NUCLEAR REACTIONS 3He(n, γ), E=0.14-2 MeV; measured absolute σ(E) for θ=90°; deduced σ(γ, p)/σ(γ, n). 4He deduced charge symmetry breaking related features. Model comparison.

doi: 10.1103/PhysRevC.48.2375
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13590.

1992OU01      Phys.Rev.Lett. 69, 1896 (1992)

J.M.L.Ouellet, H.C.Evans, H.W.Lee, J.R.Leslie, J.D.MacArthur, W.McLatchie, H.-B.Mak, P.Skensved, J.L.Whitton, X.Zhao, T.K.Alexander

12C(α, γ)16O Cross Sections at Stellar Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm)=1.37-2.98 MeV; measured σ(E), Iγ(θ); deduced E1, E2 contributions, astrophysical S-factor. Three-level R-matrix method, cluster model analysis.

doi: 10.1103/PhysRevLett.69.1896
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0104.

1990RA23      Phys.Rev. C42, R2275 (1990)

T.J.Radcliffe, T.K.Alexander, G.C.Ball, H.C.Evans, J.R.Leslie, H.-B.Mak, W.McLatchie, P.Skensved, A.T.Stewart

Search for Resonances in the Electron-Positron Annihilation-in-Flight Cross Section between 1 and 4 MeV

NUCLEAR REACTIONS 19F(p, α), E=1.27 MeV; measured e+-spectra in Ge following 16O-decay; deduced e+e- annihilation-in-flight σ.

doi: 10.1103/PhysRevC.42.R2275
Citations: PlumX Metrics

1989CL02      Nucl.Phys. A493, 293 (1989)

E.T.H.Clifford, E.Hagberg, J.C.Hardy, H.Schmeing, R.E.Azuma, H.C.Evans, V.T.Koslowsky, U.J.Schrewe, K.S.Sharma, I.S.Towner

The Decay of 20Na: Measurements of isospin mixing and the weak vector coupling constant as well as other new decay data

RADIOACTIVITY 20Na [from 12C(10B, 2n), mass separation]; measured β+ rays, β-delayed Eα, Iα, Eγ, Iγ, T1/2, I(Eγ), (βα)-coin; deduced ft values, βνα-triple correlation coefficients, vector weak coupling constants. 20Ne deduced branching ratios, Gamow-Teller matrix elements, levels, isospin mixing amplitudes. Natural target, Ge(Li), Si surface barrier detectors, NE102A plastic scintillator-Si surface barrier detector telescopes.

doi: 10.1016/0375-9474(89)90399-0
Citations: PlumX Metrics

1989SH10      Nucl.Instrum.Methods Phys.Res. A275, 123 (1989)

K.S.Sharma, H.Schmeing, H.C.Evans, E.Hagberg, J.C.Hardy, V.T.Koslowsky

The Direct Determination of the Masses of Unstable Atoms with the Chalk River On-Line Isotope Separator

ATOMIC MASSES 72Br, 63Ga; measured masses. On-line isotope separator.

doi: 10.1016/0168-9002(89)90342-2
Citations: PlumX Metrics

1988KR06      Phys.Rev.Lett. 60, 1475 (1988)

R.M.Kremer, C.A.Barnes, K.H.Chang, H.C.Evans, B.W.Filippone, K.H.Hahn, L.W.Mitchell

Coincidence Measurement of the 12C(α, γ)16O Cross Section at Low Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm)=1.29-3 MeV; measured γ-spectra, γ(recoil)-coin; deduced γ yields, dipole capture σ(E), S-factor vs E.

doi: 10.1103/PhysRevLett.60.1475
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1629.

1987KO33      Nucl.Phys. A472, 408 (1987)

V.T.Koslowsky, R.E.Azuma, H.C.Evans, E.Hagberg, J.C.Hardy, J.R.Leslie, H.Schmeing, C.Virtue

The Precise Determination of some γ-Ray Transition Energies in 26Al, 27Al and 55Co

NUCLEAR REACTIONS 25Mg(p, γ), E=1195 keV; 26Mg(p, γ), E=2141, 2220 keV; 54Fe(p, γ), E=1803, 1887 keV; measured Eγ. 26,27Al, 55Co deduced γ-ray transition energies. Enriched targets, Ge(Li) detector.

doi: 10.1016/0375-9474(87)90040-6
Citations: PlumX Metrics

1987PA07      Phys.Rev. C35, 1119 (1987)

S.A.Page, H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, W.McLatchie, P.Skensved, S.-S.Wang, H.-B.Mak, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford

Weak Pion-Nucleon Coupling Strength: New constraint from parity mixing in 18F

NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured γ CP; deduced weak pion-nucleon coupling strength. 19F levels deduced parity mixing.

doi: 10.1103/PhysRevC.35.1119
Citations: PlumX Metrics

1985EV03      Phys.Rev.Lett. 55, 791 (1985)

H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, S.A.Page, P.Skensved, S.-S.Wang, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford

Parity Mixing of 0+ and 0- Levels in 18F

NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured Eγ, Iγ, γ CP; deduced weak pion-nucleon coupling constant. 18F transition deduced parity nonconserving matrix element.

doi: 10.1103/PhysRevLett.55.791
Citations: PlumX Metrics

1984EV01      Can.J.Phys. 62, 1139 (1984)

H.C.Evans, I.P.Johnstone, J.R.Leslie, W.McLatchie, H.-B.Mak, P.Skensved, T.K.Alexander

The Branching Ratio in the Decay of 7Be

RADIOACTIVITY 7Be(EC) [from 10B(p, α), E=2 MeV]; measured Eγ, Iγ; deduced vector coupling constant G(A). 7Li level deduced EC-branching ratio.

NUCLEAR REACTIONS 10B(p, α), E=2 MeV; measured Eγ, Iγ, recoil σ(E(7Be)), σ(Eα). 7Li level deduced EC-decay branching ratio.

doi: 10.1139/p84-158
Citations: PlumX Metrics

1983CL01      Phys.Rev.Lett. 50, 23 (1983)

E.T.H.Clifford, J.C.Hardy, H.Schmeing, R.E.Azuma, H.C.Evans, T.Faestermann, E.Hagberg, K.P.Jackson, V.T.Koslowsky, U.J.Schrewe, K.S.Sharma, I.S.Towner

Kinematic Shifts in the β-Delayed Particle Decay of 20Na, and the β-ν Angular Correlation

RADIOACTIVITY 20Na(β+), (EC) [from 12C(10B, 2n), E=50 MeV]; measured βν(θ), βνα-coin; deduced β-delayed α-particle kinematic shifts, triple correlation coefficient; deduced superallowed β-decay vector weak coupling constant.

doi: 10.1103/PhysRevLett.50.23
Citations: PlumX Metrics

1983KO22      Nucl.Phys. A405, 29 (1983)

V.T.Koslowsky, E.Hagberg, J.C.Hardy, R.E.Azuma, E.T.H.Clifford, H.C.Evans, H.Schmeing, U.J.Schrewe, K.S.Sharma

The Half-Lives of 26mAl, 34Cl, 38mK: Precision measurements with isotope-separated samples

RADIOACTIVITY 26mAl(β+) [from 12C(16O, pn)]; 34Cl(β+) [from 12C(28Si, 3p3n)]; 38mK(β+) [from 12C(28Si, pn)]; measured T1/2. 4π gas proportional counter, mass separated sources.

doi: 10.1016/0375-9474(83)90321-4
Citations: PlumX Metrics

1983LE25      Nucl.Phys. A410, 93 (1983)

R.Leavitt, H.C.Evans, G.T.Ewan, H.-B.Mak, R.E.Azuma, C.Rolfs, K.P.Jackson

Isospin Mixing in 2- Levels in 16O

NUCLEAR REACTIONS 15N(p, α), (p, p), E=0.43, 0.9 MeV; measured σ(E, Eα, θ), σ(E, Ep, θ). 16O resonances deduced Γα, Γp. Differentially pumped enriched 13N gas target.

doi: 10.1016/0375-9474(83)90403-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0082.

1982EV01      Nucl.Instrum.Methods 192, 143 (1982)

H.C.Evans, G.T.Ewan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, R.C.Turnock, M.B.Woods

A Cryopumped Transmission Gas Target for Nuclear Structure Studies

NUCLEAR REACTIONS 14N(α, α)(α, γ), E ≈ 1517.5-1535 keV; measured σ(θ, E), σ(Eγ). 16O(α, γ), E=3.020, 3.036 MeV; measured Eγ, Iγ. 20Ne deduced E2 transition strength. Differentially pumped transmission gas target.

doi: 10.1016/0029-554X(82)90816-3
Citations: PlumX Metrics

1982HA32      Nucl.Phys. A383, 109 (1982)

E.Hagberg, J.C.Hardy, H.Schmeing, H.C.Evans, U.J.Schrewe, V.T.Koslowsky, K.S.Sharma, E.T.H.Clifford

The Decay of a New Nuclide: 71Br

RADIOACTIVITY 71Br [from 40Ca(35Cl, 2n2p), mass separation]; measured T1/2, Eγ, Iγ, γγ-coin. 71Se deduced levels, T1/2, transition, possible J, π, γ-multipolarity. Ge(Li), Ge detectors.

doi: 10.1016/0375-9474(82)90079-3
Citations: PlumX Metrics

1980MA26      Nucl.Phys. A343, 79 (1980)

H.-B.Mak, G.T.Ewan, H.C.Evans, J.D.MacArthur, W.McLatchie, R.E.Azuma

The Alpha Widths of the 5603, 5605 and 5668 keV States in 18F

NUCLEAR REACTIONS 14N(α, α), E=1.5, 1.6 MeV; measured σ(θ, Eα). 18F resonances deduced Γα. R-matrix formalism. Differentially pumped natural nitrogen gas target.

doi: 10.1016/0375-9474(80)90641-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1279.

1980MA27      Phys.Rev. C22, 356 (1980)

J.D.MacArthur, H.C.Evans, J.R.Leslie, H.-B.Mak

First Two Members of the K=0- Band in 20Ne

NUCLEAR REACTIONS 16O(α, α), E=1305-1330 keV, 2950-3075 keV; measured σ(E, θ); 16O(α, γ), E=1.37, 2.6, 2.9, 3.036 MeV; measured σ(E), Eγ. 20Ne resonances deduced Γα, B(λ), Γγ.

NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U; calculated binding energies. Energy density formalism, generalized Thomas-Fermi form, variational procedure.

doi: 10.1103/PhysRevC.22.356
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0693.

1979SI10      Can.J.Phys. 57, 781 (1979)

K.N.Sinha, A.G.Hwang, H.-B.Mak, H.C.Evans

A Study of the 34S(α, γ)38Ar Reaction

NUCLEAR REACTIONS 34S(α, γ), E=2-3.5 MeV; measured σ, Eγ, Iγ. 38Ar deduced levels, J, γ-branching, transition strength, δ, resonance strength.

doi: 10.1139/p79-110
Citations: PlumX Metrics

1978MA30      Nucl.Phys. A304, 210 (1978)

H.-B.Mak, H.C.Evans, G.T.Ewan, J.D.Macarthur

The 18O(p, α)15N Cross Section at Low Energies

NUCLEAR REACTIONS 18O(p, α), E=240-700 keV; measured σ(E, θ); deduced S.

doi: 10.1016/0375-9474(78)90104-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1917.

1976MA40      Phys.Rev. C14, 1320 (1976)

D.J.Martin, H.C.Evans, J.A.Szucs

γ-Ray Decay of the First T = 2 States in 36Ar

NUCLEAR REACTIONS 35Cl(p, γ), E ≈ 2410 keV; 27Al(p, γ), E ≈ 0.991 keV; measured σ(E, Eγ, θ). 36Ar deduced levels, γ-branching. 28Si level deduced S. T=2 state systematics.

doi: 10.1103/PhysRevC.14.1320
Citations: PlumX Metrics

1976MC12      Nucl.Phys. A273, 477 (1976)

A.B.McDonald, H.B.Mak, H.C.Evans, G.T.Ewan, H.B.Trautvetter

Isospin-Forbidden Particle Decays in Light Nuclei (III). Decay Widths of the Lowest T = 3/2 Level of 21Ne

NUCLEAR REACTIONS 17O(α, n), (α, nγ), E=1.4-2.3 MeV; measured n, γ yields. 21Ne deduced T=3/2 levels, Γ, Γα, Γn. Enriched target.

doi: 10.1016/0375-9474(76)90605-9
Citations: PlumX Metrics

1975MA34      Phys.Rev. C12, 1158 (1975)

H.-B.Mak, H.C.Evans, G.T.Ewan, A.B.McDonald, T.K.Alexander

Radiative Decay of the Second Excited State of 12C

NUCLEAR REACTIONS 13C(3He, α), E=4.0 MeV; measured α-12C coin. 12C level deduced Γ(rad)/Γ. Enriched target.

doi: 10.1103/PhysRevC.12.1158
Citations: PlumX Metrics

1975SI08      Nucl.Phys. A243, 1 (1975)

S.H.Sie, G.G.Frank, H.C.Evans

Perturbed Angular Distribution in 53Mn Following Resonant Proton Capture

NUCLEAR REACTIONS 52Cr(p, γ), Ep=1.724 MeV; measured Iγ(θ, H). 53Mn level deduced g. Natural target.

doi: 10.1016/0375-9474(75)90017-2
Citations: PlumX Metrics

1971RO33      Phys.Lett. 37B, 65 (1971)

D.W.O.Rogers, K.W.Allen, H.C.Evans, N.A.Jelley, A.E.Litherland, B.Y.Underwood

The 5- Resonance in the 16O(α, γ)20Ne Reaction at E = 4.65 MeV

NUCLEAR REACTIONS 16O(α, γ), E approx 4.6 MeV; measured σ(E;Eγ). 20Ne deduced resonance, level-width, J, π, γ-branching.

doi: 10.1016/0370-2693(71)90572-7
Citations: PlumX Metrics

1971SI29      Nucl.Instrum.Methods 97, 475 (1971)

B.P.Singh, H.C.Evans

Relative Efficiency of Ge(Li) Gamma Ray Detectors from 0.5 to 12 MeV

RADIOACTIVITY 56Co; measured Iγ. Ge(Li) detectors.

NUCLEAR REACTIONS 27Al(p, γ), 31P(p, γ), E=992 keV, 1248 keV; measured σ(Eγ, θ(γ)). 23Na, 39K, (p, γ), E=resonance; measured σ(Eγ, θ(γ)). 32S deduced levels, γ-branching. 24Mg, 28Si, 40Ca deduced branching ratios.

doi: 10.1016/0029-554X(71)90249-7
Citations: PlumX Metrics

1970CE02      Phys.Rev.Lett. 24, 1128 (1970)

J.Cerny, C.U.Cardinal, H.C.Evans, K.P.Jackson, N.A.Jelley

49Fe: A New T(z) = -3/2 Delayed-Proton Emitter

RADIOACTIVITY 49Fe[from 40Ca(12C, 3n)]; measured T1/2, delayed proton spectrum. 33Ar; measured delayed proton spectrum.

NUCLEAR REACTIONS 24Mg, 28Si(12C, 3n), 40Ca(12C, 3n), E=65 MeV; measured delayed proton spectrum.

doi: 10.1103/PhysRevLett.24.1128
Citations: PlumX Metrics

1970HA04      Can.J.Phys. 48, 35 (1970)

O.Hausser, B.W.Hooton, D.Pelte, T.K.Alexander, H.C.Evans

Measurement of the Reorientation Effect in 24Mg

NUCLEAR REACTIONS 24Mg(35Cl, 35Cl'γ), E=62 MeV; measured σ(E(35Cl'), Eγ, E(24Mg'), θ(γ), θ(24Mg'), phi). 24Mg deduced quadrupole moment, level-width, E2 matrix element.

1970HA24      Nucl.Phys. A150, 417 (1970)

O.Hausser, D.Pelte, T.K.Alexander, H.C.Evans

Reorientation Measurements in Even Titanium Isotopes

NUCLEAR REACTIONS 46,48Ti(35Cl, 35Cl'γ), E=70.35-74 MeV; 50Ti(32S, 32S'γ), E=67 MeV; measured Coulomb excitation, σ(E, Eγ, θ). 46,48,50Ti, 32S levels deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(70)90960-7
Citations: PlumX Metrics

1970HA30      Izv.Akad.Nauk SSSR, Ser.Fiz. 34, 909 (1970); Bull.Acad.Sci.USSR, Phys.Ser. 34, 811 (1971)

O.Hausser, B.W.Hooton, D.Pelte, T.K.Alexander, H.C.Evans

Reorientation in 24Mg

NUCLEAR REACTIONS 24Mg(35Cl, 35Cl'γ), E=62 MeV; measured σ(ecl', Eγ, θ). 24Mg level deduced quadrupole moment.

1970JA22      Phys.Lett. 33B, 281 (1970)

K.P.Jackson, C.U.Cardinal, H.C.Evans, N.A.Jelley, J.Cerny

53Co-m: A Proton-Unstable Isomer

NUCLEAR REACTIONS Ca(16O, 2np), E < 81 MeV; measured σ(E), delayed-p spectrum, (16O)(γ)-delay. 53mCo deduced T1/2.

doi: 10.1016/0370-2693(70)90269-8
Citations: PlumX Metrics

1970MO29      Can.J.Phys. 48, 2683 (1970)

C.F.Monahan, H.C.Evans, J.H.Montague, W.R.Paulson, W.M.Zuk

Transition Rates in 29P

NUCLEAR REACTIONS 28Si(p, γ), E=1-5 MeV; measured Doppler shift attenuation, σ(E;Eγ, θ(γ)). 29P deduced resonances, J, π, γ-branching, γ-mixing. 29P levels deduced T1/2.

doi: 10.1139/p70-332
Citations: PlumX Metrics

1969HA06      Phys.Rev.Letters 22, 359(1969)

O.Hausser, B.W.Hooton, D.Pelte, T.K.Alexander, H.C.Evans

Measurement of the Static Quadrupole Moment of the First Excited State In 24Mg

NUCLEAR REACTIONS 24Mg(35Cl, 35Cl'γ), E=62 MeV; measured σ(Eγ, θ). 24Mg levels deduced B(E2), quadrupole moment.

doi: 10.1103/PhysRevLett.22.359
Citations: PlumX Metrics

1969HA17      Can.J.Phys. 47, 1065 (1969)

O.Hausser, D.Pelte, T.K.Alexander, H.C.Evans

Coulomb Excitation of 35Cl Projectiles

NUCLEAR REACTIONS 12C, 24Mg(35Cl, 35Cl'γ), E = 51-61 MeV; measured Eγ, Iγ(θ), Doppler-shift attenuation. 35Cl deduced levels, T1/2, γ-mixing, γ-branching, transition strengths. Ge(Li) detector.

1969HA31      Phys.Rev.Letters 23, 320 (1969)

O.Hausser, T.K.Alexander, D.Pelte, B.W.Hooton, H.C.Evans

Coulomb Excitation of 28Si Projectiles

NUCLEAR REACTIONS 62Ni(28Si, 28Si), E=70 MeV; measured σ(E(28Si), E(62Ni), Eγ). 28Si, 62Ni levels deduced quadrupole moment.

doi: 10.1103/PhysRevLett.23.320
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1969PE08      Phys.Letters 29B, 660 (1969)

D.Pelte, O.Hausser, T.K.Alexander, B.W.Hooton, H.C.Evans

Coulomb Excitation of the First Excited State of 28Si

NUCLEAR REACTIONS 28Si(32S, 32S'γ), E=60 MeV; measured σ, σ(Eγ, θ(γ)), Doppler broadening. 28Si level deduced T1/2, quadrupole moment. Ge(Li) detector.

doi: 10.1016/0370-2693(69)90103-8
Citations: PlumX Metrics

1969PE11      Can.J.Phys. 47, 1929 (1969)

D.Pelte, O.Hausser, T.K.Alexander, H.C.Evans

Coulomb Excitation of 24Mg with 35Cl Ions

NUCLEAR REACTIONS 24Mg(35Cl, 35Cl'γ), E = 52, 57, 61 MeV; measured σ(Eγ, θ(γ)). 24Mg level deduced B(E2), quadrupole moment. Ge(Li) detector.

doi: 10.1139/p69-243
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1965EV03      Can.J.Phys. 43, 82 (1965)

H.C.Evans, M.A.Eswaran, H.E.Gove, A.E.Litherland, C.Broude

Lifetimes of the Low-Lying Levels of 20Ne

NUCLEAR STRUCTURE 20Ne, 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p65-007
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