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1997HA06 Phys.Rev. C55, 1101 (1997)

G.Hackman, S.M.Mullins, D.Haslip, S.Flibotte, J.A.Kuehner, J.C.Waddington, R.M.Clark, S.Pilotte

Neutron Excitations and Interactions above the N = 80 Superdeformed Closed Shell: Superdeformation in ¹⁴⁴Eu

NUCLEAR REACTIONS ¹²²Sn(²⁷Al, 5n), E=142 MeV; measured γγ-coin. ¹⁴⁴Eu deduced levels, J, π, superdeformed bands, configuration.

doi: 10.1103/PhysRevC.55.1101
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1995FL01 Nucl.Phys. A584, 373 (1995)

S.Flibotte, G.Hackman, I.Ragnarsson, Ch.Theisen, H.R.Andrews, G.C.Ball, C.W.Beausang, F.A.Beck, G.Belier, M.A.Bentley, T.Byrski, D.Curien, G.de France, D.Disdier, G.Duchene, B.Haas, D.S.Haslip, V.P.Janzen, P.M.Jones, B.Kharraja, J.A.Kuehner, J.C.Lisle, J.C.Merdinger, S.M.Mullins, E.S.Paul, D.Prevost, D.C.Radford, V.Rauch, J.F.Smith, J.Styczen, P.J.Twin, J.P.Vivien, J.C.Waddington, D.Ward, K.Zuber

Multi-Particle Excitations in the Superdeformed ¹⁴⁹Gd Nucleus

NUCLEAR REACTIONS ¹²⁴Sn(³⁰Si, 5n), E=158 MeV; measured Eγ, Iγ, γn-coin. ¹⁴⁹Gd deduced high-spin levels, J, π, superdeformed bands. Compton-suppressed hyperpure Ge detector array. Nilsson-Strutinsky cranking model calculations.

doi: 10.1016/0375-9474(94)00450-2
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1993FL03 Phys.Rev.Lett. 71, 688 (1993)

S.Flibotte, G.Hackman, Ch.Theisen, H.R.Andrews, G.C.Ball, C.W.Beausang, F.A.Beck, G.Belier, M.A.Bentley, T.Byrski, D.Curien, G.de France, D.Disdier, G.Duchene, P.Fallon, B.Haas, V.P.Janzen, P.M.Jones, B.Kharraja, J.A.Kuehner, J.C.Lisle, J.C.Merdinger, S.M.Mullins, E.S.Paul, D.Prevost, D.C.Radford, V.Rauch, J.F.Smith, J.Styczen, P.J.Twin, J.P.Vivien, J.C.Waddington, D.Ward, K.Zuber

Multiparticle Excitations and Identical Bands in Superdeformed ¹⁴⁹Gd Nucleus

NUCLEAR REACTIONS ¹²⁴Sn(³⁰Si, 5n), E=158 MeV; measured γγ-coin. ¹⁴⁹Gd deduced levels, J, π, superdeformed bands.

doi: 10.1103/PhysRevLett.71.688
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1993GA10 Phys.Rev.Lett. 71, 231 (1993)

A.Galindo-Uribarri, H.R.Andrews, G.C.Ball, T.E.Drake, V.P.Janzen, J.A.Kuehner, S.M.Mullins, L.Persson, D.Prevost, D.C.Radford, J.C.Waddington, D.Ward, R.Wyss

First Evidence for the Hyperdeformed Nuclear Shape at High Angular Momentum

NUCLEAR REACTIONS ¹²⁰Sn(³⁷Cl, xnp), E=187 MeV; measured γγ-, γγ(particle)-coin. ^152,153Dy deduced levels, γ-multipolarity, band structure, moment of inertia, hyperdeformation evidence.

doi: 10.1103/PhysRevLett.71.231
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1993HA03 Phys.Rev. C47, R433 (1993)

G.Hackman, S.M.Mullins, J.A.Kuehner, D.Prevost, J.C.Waddington, A.Galindo-Uribarri, V.P.Janzen, D.C.Radford, N.Schmeing, D.Ward

Superdeformed Band in ¹⁴²Sm

NUCLEAR REACTIONS ¹²⁴Sn(²⁴Mg, xn), E=145 MeV; measured γγ-coin, Eγ, Iγ. ¹⁴²Sm deduced superdeformed rotational band, continuum, dynamic moment of inertia.

doi: 10.1103/PhysRevC.47.R433
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1993HA19 Nucl.Phys. A561, 251 (1993)

B.Haas, V.P.Janzen, D.Ward, H.R.Andrews, D.C.Radford, D.Prevost, J.A.Kuehner, A.Omar, J.C.Waddington, T.E.Drake, A.Galindo-Uribarri, G.Zwartz, S.Flibotte, P.Taras, I.Ragnarsson

Studies of Superdeformation in the Gadolinium Nuclei

NUCLEAR REACTIONS ^120,122,124Sn(²⁸Si, xn), (²⁹Si, xn), (³⁰Si, xn), E=155 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. ^{145,146,147,148,149}Gd deduced, γ-multipliplicities, J, π, levels, superdeformed bands. Compton-suppressed hyperpure Ge detector array, 4π-bismuth germanate ball. Cranked shell-model-Strutinsky calculations.

doi: 10.1016/0375-9474(93)90153-O
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1992LA07 Phys.Lett. 279B, 239 (1992)

T.Lauritsen, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, J.A.Kuehner, D.Prevost, J.C.Waddington, U.Garg, W.Reviol, D.Ye, M.W.Drigert

Dynamic Moment of Inertia of the ¹⁹²Hg Superdeformed Band at High Rotational Frequencies

NUCLEAR REACTIONS ¹⁶⁰Gd(³⁶S, 4n), E=154-167 MeV; measured γγγ-coin. ¹⁹²Hg deduced superdeformed states, relative Iγ, increasing dynamic moment of inertia.

doi: 10.1016/0370-2693(92)90386-I
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1991AL06 Nucl.Phys. A526, 407 (1991)

T.K.Alexander, G.C.Ball, J.S.Forster, I.S.Towner, J.R.Leslie, H.-B.Mak, J.Johansson, J.A.Kuehner, J.C.Waddington

The l-Forbidden M1 Decay of the 2522 keV Level in ³⁹K

NUCLEAR REACTIONS ⁴He(³⁹K, α), E=100 MeV; measured Doppler shift attenuation, αγ-coin. ³⁹K levels deduced T_1/2, B(M1).

doi: 10.1016/0375-9474(91)90293-F
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1989HA26 Phys.Rev. C40, 1234 (1989)

E.D.Hackett, J.A.Kuehner, J.C.Waddington, G.D.Jones

Spin of the ²¹⁹Ra Ground State

RADIOACTIVITY ²²³Th(α) [from ²⁰⁸Pb(¹⁸O, 3n), E=83 MeV]; ²¹⁹Ra [from ²²³Th(α-decay)]; measured αγ(θ). ²¹⁵Rn, ²¹⁹Ra level deduced possible J, π.

doi: 10.1103/PhysRevC.40.1234
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1989JO04 Phys.Rev.Lett. 63, 2200 (1989)

J.K.Johansson, H.R.Andrews, T.Bengtsson, A.Djaafri, T.E.Drake, S.Flibotte, A.Galindo-Uribarri, D.Horn, V.P.Janzen, J.A.Kuehner, S.Monaro, N.Nadon, S.Pilotte, D.Prevost, D.C.Radford, I.Ragnarsson, P.Taras, A.Tehami, J.C.Waddington, D.Ward, S.Aberg

Multiple Superdeformed Bands in ¹⁵³Dy

NUCLEAR REACTIONS ¹²⁴Sn(³⁴S, 5n), E not given; measured γγγ-coin, sum spectra. ¹⁵³Dy deduced levels, J, π, moment of inertia, band structure, deformation, superdeformation features.

doi: 10.1103/PhysRevLett.63.2200
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1988VE07 Phys.Rev. C38, 2503 (1988)

M.C.Vetterli, J.A.Kuehner, C.Bamber, N.Davis, A.J.Trudel, H.R.Weller, R.M.Whitton

Vector Analyzing Powers for ¹H(d(pol), γ)³He and ²H(p(pol), γ)³He

NUCLEAR REACTIONS ¹H(polarized d, γ), E=6 MeV; ²H(polarized p, γ), E=3 MeV; measured σ(θ), analyzing power; deduced S=(3/2) capture strength.

doi: 10.1103/PhysRevC.38.2503
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1986BA47 Phys.Rev. C34, 1236 (1986)

C.Bamber, N.J.Davis, J.A.Kuehner, A.A.Pilt, A.J.Trudel, M.C.Vetterli, G.D.Jones

Spin-Parity Measurements in ^44,46Sc

NUCLEAR REACTIONS ^46,48Ti(polarized d, α), E=7, 8, 8.25, 9.25, 9.75 MeV; measured σ(Eα), tensor analyzing power vs E. ^44,46Sc deduced levels, J, π. Magnetic spectrometer.

doi: 10.1103/PhysRevC.34.1236
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1986DA09 Phys.Rev. C33, 1799 (1986)

N.J.Davis, J.A.Kuehner, A.J.Trudel, C.Bamber

0^- State at Low Excitation Energy in ²⁶Al

NUCLEAR REACTIONS ²⁸Si(polarized d, α), E=8, 8.5, 9, 9.5, 12 MeV; measured T₂₀(0°). ²⁶Al level deduced J, π.

doi: 10.1103/PhysRevC.33.1799
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1985DA15 Phys.Rev. C32, 713 (1985)

N.J.Davis, J.A.Kuehner, A.A.Pilt, A.J.Trudel, M.C.Vetterli, C.Bamber, E.K.Warburton, J.W.Olness, S.Raman

States of ³⁸S from the ³⁶S(t, p)³⁸S Reaction

NUCLEAR STRUCTURE ³⁸S; calculated levels. Shell, weak coupling models.

NUCLEAR REACTIONS ³⁶S(t, p), E=18 MeV; measured σ(θ). ³⁸S deduced levels J, π. Enriched target. DWBA analysis.

doi: 10.1103/PhysRevC.32.713
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1985VE02 Phys.Rev.Lett. 54, 1129 (1985)

M.C.Vetterli, J.A.Kuehner, A.J.Trudel, C.L.Woods, R.Dymarz, A.A.Pilt, H.R.Weller

Measurement of T₂₀ for the Reaction ¹H(d(pol), γ)³He and D-State Effects in ³He

NUCLEAR REACTIONS ¹H(polarized d, γ), E=19.8 MeV; measured tensor analyzing power T₂₀(θ). ³He deduced D-state effects.

doi: 10.1103/PhysRevLett.54.1129
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1984SH16 Nucl.Phys. A425, 411 (1984)

R.Shang, A.A.Pilt, M.C.Vetterli, A.J.Trudel, J.A.Kuehner

Energy Levels of ⁵⁶Co Studied by the ⁵⁸Ni(d(pol), α)⁵⁶Co Reaction near 0°

NUCLEAR REACTIONS ⁵⁸Ni(polarized d, α), E=6.75-9.5 MeV; measured T₂₀(θ); ⁵⁸Ni(d, α), E=7 MeV; measured σ(E(α), θ). ⁵⁶Co levels deduced J, π.

doi: 10.1016/0375-9474(84)90015-0
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1984VE07 Aust.J.Phys. 37, 123 (1984)

W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds

Coulomb Excitation of the 2.615 MeV (3^-) and 4.086 MeV (2⁺) States of ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹²C, ¹²C'), E=53-58 MeV; ²⁰⁸Pb(¹⁶O, ¹⁶O'), E=57-76 MeV; measured Coulomb excitation. ²⁰⁸Pb levels deduced B(λ), quadrupole moment.

doi: 10.1071/PH840123
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1983SP02 Phys.Lett. 128B, 29 (1983)

R.H.Spear, W.J.Vermeer, M.T.Esat, J.A.Kuehner, A.M.Baxter, S.Hinds

An Improved Determination of the Quadrupole Moment of the First Excited State of ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹²C, ¹²C'), E=75, 90 MeV; ²⁰⁸Pb(¹⁶O, ¹⁶O'), E=80-171.6 MeV; analyzed Coulomb excitation data. ²⁰⁸Pb level deduced static quadrupole moment, B(E3).

doi: 10.1016/0370-2693(83)90067-9
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1983VE01 Phys.Lett. 122B, 23 (1983)

W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds

Electric Quadrupole Moment of the First Excited State of ¹²C

NUCLEAR REACTIONS ²⁰⁸Pb(¹²C, ¹²C'), E=53, 54, 56, 58 MeV; ²⁰⁸Pb(¹⁶O, ¹⁶O'), E=72 MeV; measured σ(E(¹²C)), σ(E(¹⁶O)), projectile Coulomb excitation. ¹²C level deduced quadrupole moment.

doi: 10.1016/0370-2693(83)91160-7
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1983WO06 Nucl.Phys. A402, 31 (1983)

C.L.Woods, J.A.Kuehner, A.A.Pilt, A.J.Trudel, M.C.Vetterli

Spin-Parity Assignments for ⁶⁶Cu Levels via the ⁶⁸Zn(d(pol), α)⁶⁶Cu Reaction

NUCLEAR REACTIONS ⁶⁸Zn(polarized d, α), E=9, 9.5, 10, 10.5 MeV; measured T₂₀(θ=4°). ⁶⁶Cu levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(83)90560-2
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1982BA55 Nucl.Phys. A390, 29 (1982)

A.M.Baxter, A.M.Mcdonald, P.G.Ikossi, J.A.Kuehner

Spin-Parity Determinations in ⁴²K from the ⁴⁴Ca(d(pol), α)⁴²K Reaction near 0°

NUCLEAR REACTIONS ⁴⁴Ca(polarized d, α), E=7, 7.25, 7.5, 7.75, 8, 8.25 MeV; measured T₂₀(θ=4°). ⁴²K deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(82)90604-2
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1982KU14 Phys.Lett. 115B, 437 (1982)

J.A.Kuehner, R.H.Spear, W.J.Vermeer, M.T.Esat, A.M.Baxter, S.Hinds

A Measurement of the Giant-Dipole-Resonance Contribution to the Coulomb Excitation of ¹⁷O

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁷O, ¹⁷O'), E=66-88 MeV; measured σ(E(¹⁷O)), projectile Coulomb excitation probability. ¹⁷O level deduced GDR contribution parameter. Modified hydrodynamic model. ²⁰⁸Pb(¹⁷O, ¹⁶O), (¹⁷O, ¹⁸O), E=66-88 MeV; measured σ(E(¹⁶O)), σ(E(¹⁸O)).

doi: 10.1016/0370-2693(82)90387-2
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1982VE11 Aust.J.Phys. 35, 283 (1982)

W.J.Vermeer, T.H.Zabel, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter

The Giant Dipole Resonance Effect in Coulomb Excitation of ¹⁰B

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁰B, ¹⁰B'), (¹⁰B, ⁹B), (¹⁰B, ¹¹B), E=32-38 MeV; measured σ(E(¹⁰B)), σ(E(⁹B)), σ(E(¹¹B)), projectile Coulomb excitation. ¹⁰B deduced virtual GDR excitation.

doi: 10.1071/PH820283
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1982WO08 Phys.Lett. 116B, 320 (1982)

P.W.Woods, R.Chapman, J.N.Mo, P.Skensved, J.A.Kuehner

Proton Orbit Sizes in ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(t, α), E=8.5, 9 MeV; ²⁰⁸Pb(t, t), E=8.5, 9, 10, 12 MeV; measured σ(θ), σ(Eα); deduced optical model parameters. ²⁰⁸Pb deduced single proton state S, rms radius, binding energy. DWBA analysis.

doi: 10.1016/0370-2693(82)90290-8
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1981PI03 Phys.Lett. 100B, 114 (1981)

A.A.Pilt, J.A.Kuehner, R.Shang, M.A.M.Shahabuddin, A.Trudel

The Selection Rule in (d, α) Reactions Leading to 0⁺ Antianalogue States in Odd-Odd Nuclei

NUCLEAR REACTIONS ⁴²Ca(d, α), E=7-10 MeV; analyzed data; deduced reaction selection rule. ⁴⁰K deduced antianalog state, J, π, configuration. Shell model.

doi: 10.1016/0370-2693(81)90755-3
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1981SH02 Phys.Rev. C23, 64 (1981)

M.A.M.Shahabuddin, J.A.Kuehner, A.A.Pilt

(t, d) Reaction on ¹²⁴Te, ¹²⁶Te, ¹²⁸Te, and ¹³⁰Te Nuclei

NUCLEAR REACTIONS ^{124,126,128,130}Te(t, d), E=16 MeV; measured σ(Ed, θ). ^{125,127,129,131}Te levels deduced L, S, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.23.64
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1981SH12 Nucl.Phys. A366, 13 (1981)

R.-C.Shang, A.A.Pilt, J.A.Kuehner, M.A.M.Shahabuddin, A.Trudel

Spin-Parity Determinations to ⁴⁰K Levels via the ⁴²Ca(d(pol), α) Reaction

NUCLEAR REACTIONS ⁴²Ca(polarized d, α), (d, α), E=7-10 MeV; measured T₂₀(Eα, θ), σ(Eα, θ). ⁴⁰K deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(81)90484-X
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1981WA03 Nucl.Phys. A356, 33 (1981)

A.Warwick, R.Chapman, J.L.Durell, J.N.Mo, J.A.Kuehner, P.Skensved

The 1h_9/2 Proton Orbit Size in ²⁰⁹Bi

NUCLEAR REACTIONS ²⁰⁹Bi(t, α), E=8.5, 9 MeV; measured σ(θ). ²⁰⁹Bi deduced rms radius, asymptotic amplitude of the 1h_9/2 proton wave function. Zero-range, finite-range DWBA analysis.

doi: 10.1016/0375-9474(81)90116-0
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1981WO05 Phys.Lett. 105B, 339 (1981)

P.Woods, R.Chapman, J.N.Mo, P.Skensved, J.A.Kuehner

The Sub-Coulomb ²⁰⁷Pb(t, d) Reaction and the (t, d) Normalization Constant

NUCLEAR REACTIONS ²⁰⁷Pb(t, d), E=8, 8.5, 9 MeV; ²⁰⁷Pb(t, t), E=8.5, 9 MeV; measured σ(θ). ²⁰⁸Pb deduced 3p_1/2 neutron orbit rms radius. DWBA analysis.

doi: 10.1016/0370-2693(81)90775-9
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1980AN15 Phys.Rev. C22, 427 (1980)

S.Angelo, A.A.Pilt, J.A.Kuehner

Spin-Parity Determinations from the ⁴⁸Ca(d, α)⁴⁶K Reaction Near 0°

NUCLEAR REACTIONS ⁴⁸Ca(polarized d, α), E=7.5, 8, 8.5, 9 MeV; measured tensor analyzing power vs θ. ⁴⁶K levels deduced J, π. Enriched target.

doi: 10.1103/PhysRevC.22.427
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1980PI04 Phys.Rev. C22, 462 (1980)

A.A.Pilt, J.A.Cameron, J.A.Kuehner

Spin-Parity Combinations and Low-Lying 2p-4h States in ⁵⁴Mn

NUCLEAR REACTIONS ⁵⁶Fe(polarized d, α), E=7.5, 8, 8.5, 9, 9.5 MeV; measured tensor analyzing power vs θ: ⁵⁶Fe(d, α), E=9 MeV; measured σ(Eα, θ). ⁵⁴Mn deduced levels, J, π. Shell model.

doi: 10.1103/PhysRevC.22.462
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1980SH03 Phys.Rev. C21, 1116 (1980)

M.A.M.Shahabuddin, A.A.Pilt, J.A.Kuehner

(t, α) Reaction on ¹²⁴Te, ¹²⁶Te, ¹²⁸Te, and ¹³⁰Te Nuclei

NUCLEAR REACTIONS ^{124,126,128,130}Te(t, α), E=16 MeV; measured σ(Eα, θ). ^{123,125,127,129}Sb levels deduced C²S. DWBA.

doi: 10.1103/PhysRevC.21.1116
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1979PI01 Phys.Rev. C19, 20 (1979)

A.A.Pilt, M.A.M.Shahabuddin, J.A.Kuehner

States in ²⁰O below 6 MeV Excitation via the ¹⁸O(t, p)²⁰O Reaction

NUCLEAR REACTIONS ¹²C(t, p), ^16,18O(t, p), E=15 MeV; measured σ(Ep, θ). ²⁰O deduced levels, J. DWBA analysis, shell model calculation. Enriched target.

doi: 10.1103/PhysRevC.19.20
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1979PI09 Phys.Rev. C20, 1186 (1979)

A.A.Pilt, J.A.Kuehner, S.J.Wilson, J.J.Simpson

¹²C(¹²C, t)²¹Na Reaction between 37 and 50 MeV

NUCLEAR REACTIONS ¹²C(¹²C, t), E=37-50 MeV; measured σ(E, Et, θ). ²¹Na deduced levels.

doi: 10.1103/PhysRevC.20.1186
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1978BA43 Nucl.Phys. A305, 213 (1978)

A.M.Baxter, P.G.Ikossi, A.M.McDonald, J.A.Kuehner

Spin-Parity Combinations in ¹⁶N from the ¹⁸O(d, α)¹⁶N Reaction

NUCLEAR REACTIONS ¹⁸O(polarized d, α), E=8.50, 9.25, 10.00, 10.30, 10.75, 11.30 MeV; measured A(Eα). ¹⁶N levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(78)90174-4
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1978IK01 Nucl.Phys. A297, 1 (1978)

P.G.Ikossi, A.M.McDonald, J.A.Kuehner

A Study of the ³⁰Si(d, α)²⁸Al Reactions

NUCLEAR REACTIONS ^28,30Si(polarized d, α), E=18.0 MeV; measured σ(θ), iT₁₁(θ). ^26,28Al levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(78)90194-X
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1978SI01 Phys.Rev.Lett. 40, 154 (1978)

J.J.Simpson, S.J.Wilson, W.R.Dixon, R.S.Storey, J.A.Kuehner

Isospin Impurity in the Compound Nucleus from a Comparison of Fluctuations in Mirror Reactions

NUCLEAR REACTIONS ¹²C(¹⁴N, t), (¹⁴N, ³He), E=39-50.2 MeV; measured σ(E), Ericson fluctuations.

doi: 10.1103/PhysRevLett.40.154
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1978VO01 Phys.Lett. 72B, 311 (1978)

P.B.Vold, D.Cline, R.N.Boyd, H.Clement, W.P.Alford, J.A.Kuehner

The Effective T = 1 Two-Particle Matrix Elements in the fp Shell

NUCLEAR REACTIONS ⁴¹Ca(polarized d, p), E=11 MeV; measured σ(Ep, θ), A(θ). ⁴²Ca deduced strength distributions.

doi: 10.1016/0370-2693(78)90126-0
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1978VO04 Nucl.Phys. A302, 12 (1978)

P.B.Vold, D.Cline, R.N.Boyd, H.Clement, W.P.Alford, J.A.Kuehner

Nuclear Spectroscopy of the (f₇/₂)², f₇/₂p₃/₂ and f₇/₂p₁/₂ Multiplets from the ⁴¹Ca(d, p)⁴²Ca Reaction

NUCLEAR REACTIONS ^40,41Ca(polarized d, p), E=11 MeV; measured σ(Ep, θ), iT₁₁(θ). ⁴²Ca deduced levels, L, π, J, S. ⁴¹Ca levels deduced S. Enriched, radioactive target.

doi: 10.1016/0375-9474(78)90284-1
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1978WE13 Phys.Rev. C18, 1120 (1978)

H.R.Weller, J.Szucs, P.G.Ikossi, J.A.Kuehner, D.T.Petty, R.G.Seyler

Elastic Scattering of Polarized Protons from ¹³C for 9.1 < E < 18.4 MeV

NUCLEAR REACTIONS ¹³C(polarized p, p), E=9.1-18.4 MeV; measured σ(E, θ). ¹³C(polarized p, p), E=10-17.5 MeV; measured A(E, θ). ¹⁴N deduced resonances.

doi: 10.1103/PhysRevC.18.1120
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1977BA68 Nucl.Phys. A291, 282 (1977)

A.M.Baxter, P.G.Ikossi, A.M.McDonald, J.A.Kuehner

Spin-Parity Combinations in ³²P from the ³⁴S(d, α)³²P Reaction

NUCLEAR REACTIONS ³⁴S(polarized d, α), E=8.25, 8.50, 8.75, 9.25, 9.50 MeV; measured T₂₀(4°). ³²P levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(77)90320-7
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1977DA01 Phys.Rev. C15, 104 (1977)

J.M.Davidson, D.M.Sheppard, P.W.Green, J.A.Kuehner

⁹²Nb Using ⁸⁹Y(α, nγ)⁹²Nb and ⁹²Zr(p, nγ)⁹²Nb

NUCLEAR REACTIONS ⁸⁹Y(α, nγ), E=7.0-12.5 MeV; ⁹²Zr(p, nγ), E=3-5 MeV; measured Eγ, σ(E, Eγ, θ), γγ-coin. ⁹²Nb deduced levels, J, π, δ. Enriched, natural targets; Ge(Li) detectors.

doi: 10.1103/PhysRevC.15.104
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1977KE16 Nucl.Phys. A289, 61 (1977)

D.T.Kelly, P.W.Green, J.A.Kuehner

Levels in ⁷¹Ge Studied with the ⁶⁸Zn(α, nγ)⁷¹Ge Reaction

NUCLEAR REACTIONS ⁶⁸Zn(α, nγ), E=8-10 MeV; measured Eγ, σ(Eγ, θ(γ)), γγ-coin. ⁷¹Ge deduced levels, J, π, δ. Enriched target. Ge(Li) detectors.

doi: 10.1016/0375-9474(77)90521-8
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1977KU02 Phys.Lett. 66B, 32 (1977)

J.A.Kuehner, J.Szucs, P.Ikossi, A.M.McDonald, D.T.Petty

Use of Tensor Polarized Deuterons in Method II Angular Correlations

NUCLEAR REACTIONS ²⁴Mg(polarized d, αγ), E=7.7, 9.3 MeV; measured γγ(θ). ²²Na levels deduced J, π, δ, λ.

doi: 10.1016/0370-2693(77)90606-2
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1976BO33 Phys.Rev. C14, 946 (1976)

R.N.Boyd, D.Elmore, H.Clement, W.P.Alford, J.A.Kuehner, G.D.Jones

Positive-Parity Levels in ⁴¹Ca Populated in the ⁴⁰Ca(d, p)⁴¹Ca(J*) Reaction

NUCLEAR REACTIONS ⁴⁰Ca(polarized d, p), E=11.0 MeV; measured σ(Ep, θ), A(θ). ⁴¹Ca positive parity levels deduced structure. CCBA analysis.

doi: 10.1103/PhysRevC.14.946
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1976PE08 Phys.Rev. C14, 12 (1976)

D.T.Petty, J.A.Kuehner, J.Szucs, P.W.Green, G.D.Jones

Tensor Analyzing Power Measurements in the ¹⁶O(d, α)¹⁴N Reaction at 0°

NUCLEAR REACTIONS ¹⁶O(polarized d, α), E=11, 12, 13, 14 MeV; measured A(θ), α-yields. ¹⁴N levels deduced J, π.

doi: 10.1103/PhysRevC.14.12
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1976PE11 Phys.Rev. C14, 908 (1976)

D.T.Petty, P.G.Ikossi, J.A.Kuehner, J.Szucs

Spin and Parity Assignments in ³⁸K via the (d, α) Reaction Near 0°

NUCLEAR REACTIONS ⁴⁰Ca(polarized d, α), E=7.5, 7.75, 8.0 MeV; measured A(θ), θ=20°. ³⁸K levels deduced J, π.

doi: 10.1103/PhysRevC.14.908
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1976WE08 Phys.Rev. C13, 1055 (1976)

H.R.Weller, J.Szucs, J.A.Kuehner, G.D.Jones, D.T.Petty

Elastic Scattering of Polarized Protons from ⁵⁶Fe in the Giant Resonance Region of ⁵⁷Co

NUCLEAR REACTIONS ⁵⁶Fe(polarized p, p), E=8-17 MeV; measured σ(E, θ), A(E, θ). Phase-shift analysis.

doi: 10.1103/PhysRevC.13.1055
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1975GR25 Phys.Rev. C12, 887 (1975)

P.W.Green, G.D.Jones, D.T.Kelly, J.A.Kuehner, D.T.Petty

γ-Ray Decay of the 9.042 and 9.806 MeV States in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E(cm)=19.3 MeV; measured σ(Eγ, θ), pγ-coin, DSA. ²³Na deduced levels, J, π, δ, γ-branching, T_1/2.

doi: 10.1103/PhysRevC.12.887
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1975JO03 Phys.Rev. C12, 132 (1975)

G.D.Jones, P.W.Green, D.T.Kelly, G.G.Frank, J.A.Kuehner

5.534 MeV Level in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E=28.2 MeV; measured pγ(θ), linear polarization. ²³Na level deduced J, π, δ, γ-branching.

doi: 10.1103/PhysRevC.12.132
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1975JO06 Phys.Lett. 59B, 236 (1975)

G.D.Jones, P.W.Green, J.A.Kuehner, D.T.Petty, J.Szucs, H.R.Weller

Identification of Jπ = 0^- Levels in Odd-Odd Nuclei and the Absolute Determination of t₂₀ for Polarized Spin-1 Beams

NUCLEAR REACTIONS ¹⁶O(polarized d, α), E=14 MeV; measured α yields. ¹⁴N level deduced J, π.

doi: 10.1016/0370-2693(75)90035-0
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1975KU15 Phys.Rev.Lett. 35, 423 (1975)

J.A.Kuehner, P.W.Green, G.D.Jones, D.T.Petty

New Technique for Parity Measurement Using Polarized Deuterons

NUCLEAR REACTIONS ¹²C(polarized d, α), E=14.5 MeV; measured σ(Eα, θ). ¹⁰B levels deduced J, π. New technique for parity determination.

doi: 10.1103/PhysRevLett.35.423
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1975SI12 Phys.Rev.Lett. 35, 23 (1975)

J.J.Simpson, S.J.Wilson, P.W.Green, J.A.Kuehner, W.R.Dixon, R.S.Storey

Identification of the 6⁺ and 8⁺ Yrast States in ⁴⁰Ca

NUCLEAR REACTIONS ²⁸Si(¹⁴N, npγ), E=34 MeV; measured σ(Eγ, θ). ⁴⁰Ca deduced levels, J, λ.

doi: 10.1103/PhysRevLett.35.23
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1975SI19 Phys.Rev. C12, 468 (1975)

J.J.Simpson, W.Dunnweber, J.P.Wurm, P.W.Green, J.A.Kuehner, W.R.Dixon, R.S.Storey

Yrast Levels in ⁴⁴Ti

NUCLEAR REACTIONS ³²S(¹⁴N, pnγ), E=26-43 MeV; measured σ(E, Eγ, θ), γγ-coin, DSA. ⁴⁴Ti deduced levels, J, π, T_1/2, λ, B(E2).

doi: 10.1103/PhysRevC.12.468
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1974GR15 Can.J.Phys. 52, 950 (1974)

H.Grawe, J.E.Cairns, M.W.Greene, J.A.Kuehner

An Investigation of Odd Parity States in ³²S

NUCLEAR REACTIONS ³¹P(p, γ), E=0.8-2.0 MeV; ^32,34S(α, α'), E=16-18 MeV; measured DSA, σ(θ), σ(Eα'), P(γ). ³²S deduced levels, J, π, T_1/2, γ-branching ratios, γ-mixing.

doi: 10.1139/p74-130
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0875.

1974GR28 Can.J.Phys. 52, 1485 (1974)

M.W.Greene, H.H.Grawe, J.A.Kuehner

Negative Parity Levels in ³⁰Si

NUCLEAR REACTIONS ²⁷Al(α, pγ), E=9, 13 MeV; measured pγ-coin, pγ(θ), Eγ, Iγ, pγ(θ), DSA. ³⁰Si deduced levels, J, π, T_1/2, γ-branching ratios, λ.

doi: 10.1139/p74-195
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1973FR07 Can.J.Phys. 51, 1155 (1973)

G.G.Frank, R.V.Elliott, R.H.Spear, J.A.Kuehner

High-Spin States in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E=27-29 MeV; measured Eγ, Iγ, σ(Ep), DSA, pγ(θ). ²³Na deduced levels, γ-branching, T_1/2, J, π.

doi: 10.1139/p73-154
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1972FR01 Phys.Rev.Lett. 28, 571 (1972)

G.G.Frank, M.W.Greene, D.T.Kelly, A.A.Pilt, J.A.Kuehner

E1 Decay of Members of the Low-Lying Kπ = 1/2^- Band in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, p), E=28.2 MeV; measured σ(Ep, Eγ, θ(pγ)), DSA. ²³Na deduced level, J, π, T_1/2, γ-branching.

doi: 10.1103/PhysRevLett.28.571
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1972GR15 Nucl.Phys. A188, 83 (1972)

M.W.Greene, J.A.Kuehner, G.C.Ball, C.Broude, J.S.Forster

Lifetime of the 5.69 MeV 5^- Levels in ³⁴S

NUCLEAR REACTIONS ³¹P(α, p), E=9.5 MeV; measured recoil distance. ³⁴S level deduced T_1/2. Natural target.

doi: 10.1016/0375-9474(72)90183-2
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1972PI03 Can.J.Phys. 50, 1286 (1972)

A.A.Pilt, R.H.Spear, R.V.Elliott, D.T.Kelly, J.A.Kuehner, G.T.Ewan, C.Rolfs

Band Structure in ²¹Ne

NUCLEAR REACTIONS ¹⁸O(α, nγ), E=5.2, 6.1 MeV; measured γγ-coin, γ-linear polarization, Iγ(θ). ²¹Ne levels deduced J, π, γ-mixing, γ-branching. Ge(Li) detectors.

doi: 10.1139/p72-176
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1971GR26 Phys.Lett. 35B, 560 (1971)

M.W.Greene, J.A.Kuehner, A.A.Pilt

The Jπ = 5^- Level in ³⁴S at 5.689 MeV

NUCLEAR REACTIONS ³¹P(α, pγ), E=9.5 MeV; measured σ(Eγ, θ(γ)), γ-linear polarization correlations. ³⁴S level deduced J, π.

doi: 10.1016/0370-2693(71)90286-3
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1971OL01 Can.J.Phys. 49, 594 (1971)

R.W.Ollerhead, G.F.R.Allen, A.M.Baxter, B.W.J.Gillespie, J.A.Kuehner

Spin-Parity Combinations in ²²Ne

NUCLEAR REACTIONS ²²Ne(α, α'), E=16.5-21.0 MeV; measured σ(Eα'). ²²Ne deduced levels, J, π.

doi: 10.1139/p71-077
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1971OL06 Can.J.Phys. 49, 2589 (1971)

R.W.Ollerhead, G.F.R.Allen, A.M.Baxter, J.A.Kuehner

Spin-Parity Combinations in ¹⁸O

NUCLEAR REACTIONS ¹⁸O(α, α'), E=20-23.4 MeV; measured σ(E;Eα'). ¹⁸O deduced levels, J, π.

doi: 10.1139/p71-309
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1971PI03 Can.J.Phys. 49, 1263 (1971)

A.A.Pilt, R.H.Spear, R.V.Elliott, J.A.Kuehner

Positive-Parity Bands in ²⁹Si

NUCLEAR REACTIONS ²⁶Mg(α, nγ), E=5.54, 6.30 MeV; measured σ(Eγ, θ), γ-linear polarization. ²⁹Si deduced levels, J, π, γ-branching, γ-mixing.

doi: 10.1139/p71-151
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1971SP02 Can.J.Phys. 49, 355 (1971)

R.H.Spear, J.E.Cairns, R.V.Elliott, J.A.Kuehner, A.A.Pilt

Concerning a Possible K = 7/2 Negative Parity Band in ²⁹Si

NUCLEAR REACTIONS ²⁶Mg(α, nγ), E=5.54, 6.30 MeV; measured σ(Eγ;θ(γ)), γ-linear polarization. ²⁹Si levels deduced J, π, γ-mixing.

doi: 10.1139/p71-041
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1970BA47 Can.J.Phys. 48, 2434 (1970)

A.M.Baxter, B.W.J.Gillespie, J.A.Kuehner

Gamma-Ray Polarization Measurements in ²²Na

NUCLEAR REACTIONS ¹⁹F(α, nγ), E=6.13, 7.00 MeV; measured σ(Eγ, θ(γ)), γ-linear polarization. ²²Na levels deduced J, π, γ-mixing. Ge(Li) detectors.

doi: 10.1139/p70-305
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1969AL01 Can.J.Phys. 47, 651(1969)

T.K.Alexander, C.Broude, A.J.Ferguson, J.A.Kuehner, A.E.Litherland, R.W.Ollerhead, P.J.M.Smulders

Lifetimes and Branching Ratios of Energy Levels of ²⁸Si. II

NUCLEAR REACTIONS ²⁵Mg(α, nγ), E=6.0-7.2 MeV; measured Eγ, Doppler broadening. ¹⁶O(¹⁶O, α), E=20-25 MeV; measured σ(Eα). ²⁸Si deduced levels, J, π, T_1/2, γ-branching. Ge(Li) detector.

doi: 10.1139/p69-085
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1969BA46 Can.J.Phys. 47, 2319 (1969)

A.M.Baxter, K.J.Cassell, J.A.Kuehner

Resonance Strengths and Decay Schemes in ²³Na(p, γ)²⁴Mg

NUCLEAR REACTIONS ²³Na(p, γ), E = 0.5-1.5 MeV; measured σ(E;Eγ), Doppler shift attenuation. ²⁴Mg deduced resonances, level-width. ²⁴Mg deduced levels, J, π, branching ratios, T_1/2.

doi: 10.1139/p69-282
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1969BA47 Can.J.Phys. 47, 2327 (1969)

A.M.Baxter, C.Mabey, B.W.J.Gillespie, J.A.Kuehner

Angular Correlations in ²³Na(p, γ)²⁴Mg

NUCLEAR REACTIONS ²³Na(p, γ), E = 1.020, 1.318 MeV; measured γγ(θ). ²⁴Mg deduced resonances, J. ²⁴Mg level deduced J, π.

doi: 10.1139/p69-283
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1968OL04 Can.J.Phys. 46, 1381 (1968)

R.W.Ollerhead, J.A.Kuehner, R.J.A.Levesque, E.W.Blackmore

Study of Levels in ²⁴Mg

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

doi: 10.1139/p68-459
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1967KU04 Can.J.Phys. 45, 1605 (1967)

J.A.Kuehner, E.Almqvist

New High-Spin Levels in ²⁰Ne

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

doi: 10.1139/p67-124
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1967LI07 Can.J.Phys. 45, 1901 (1967)

A.E.Litherland, R.W.Ollerhead, P.J.M.Smulders, T.K.Alexander, C.Broude, A.J.Ferguson, J.A.Kuehner

Study of Some ²⁰Ne Levels by Radiative Capture

NUCLEAR STRUCTURE ¹⁶O, ²⁰Ne, ⁴He; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p67-146
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1966KU03 Phys.Letters 20, 301 (1966)

J.A.Kuehner, R.W.Ollerhead

The Observation of an 8+ Level in ²⁰Ne

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

doi: 10.1016/0031-9163(66)90374-X
Citations: PlumX Metrics

1966LE07 Can.J.Phys. 44, 1087 (1966)

R.J.A.Levesque, R.W.Ollerhead, E.W.Blackmore, J.A.Kuehner

Properties of Levels at 6.69 and 6.88-6.89 MeV in ²⁸Si

NUCLEAR STRUCTURE ²⁸Si; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p66-091
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1965KU01 Bull.Am.Phys.Soc. 10, No.1, 37, CC8 (1965)

J.A.Kuehner, E.Almqvist

High-Spin Levels of Mg²⁴

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

1965PE01 Bull.Am.Phys.Soc. 10, No.1, 37, CC6 (1965)

J.D.Pearson, T.K.Alexander, C.Broude, A.E.Litherland, J.A.Kuehner, E.Almqvist

Comparison Between the F¹⁹+d and C¹²+C¹² Reaction Leading to Levels in Ne²⁰

NUCLEAR STRUCTURE ¹²C, ¹⁹F, ²⁰Ne; measured not abstracted; deduced nuclear properties.

1964AL15 Nucl. Phys. 55, 145 (1964)

E.Almqvist, J.A.Kuehner

5.63 and 5.80 MeV Levels of Ne²⁰; De-excitation Branching

NUCLEAR REACTIONS ¹²C(¹²C, α) , E(¹²C)=16-22 MeV; measured I(²⁰Ne)/I(α'), α-spectrum. ²⁰Ne deduced levels, level-width γ/level-width.

doi: 10.1016/0029-5582(64)90134-8
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1964AL17 Phys. Rev. 136, B84 (1964)

E.Almqvist, J.A.Kuehner, D.McPherson, E.W.Vogt

Effects of Sample Size and Statistical Weights on Fluctuations in the C¹²(C¹², α)Ne²⁰ Reactions

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

doi: 10.1103/PhysRev.136.B84
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1964HI02 Can.J.Phys. 42, 153 (1964)

B.Hird, J.A.Kuehner, E.Almqvist, C.Brassard

Spin-Parity Combinations of Levels in Mg²⁴ below 9.6-MeV Excitation

NUCLEAR STRUCTURE ¹²C, ²⁴Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p64-012
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1964KU03 Can.J.Phys. 42, 477 (1964)

J.A.Kuehner, J.D.Pearson

New 5- and 6+ States in Ne²⁰

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

doi: 10.1139/p64-043
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1964KU04 Bull.Am.Phys.Soc. 9, No.4, 430, EA9 (1964); Priv.Comm. (1964)

J.A.Kuehner, E.Almqvist

New α-Emitting Levels in ²⁰Ne

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

1964PE02 Can.J.Phys. 42, 489 (1964)

J.D.Pearson, E.Almqvist, J.A.Kuehner

Levels in Ne²⁰ from the C¹²(C¹², α)Ne²⁰ Reaction

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

doi: 10.1139/p64-044
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1964VO03 Phys.Rev. 136, B99 (1964)

E.W.Vogt, D.McPherson, J.A.Kuehner, E.Almqvist

Average Cross Sections for the C¹²(C¹², α)Ne²⁰ Reactions

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

doi: 10.1103/PhysRev.136.B99
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1963AL07 Phys.Rev. 130, 1140 (1963)

E.Almqvist, D.A.Bromley, J.A.Kuehner, B.Whalen

Spins and Partial Widths of Quasimolecular Resonances in C¹² + C¹² Interactions

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

doi: 10.1103/PhysRev.130.1140
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1963AL23 Conf. Compd.Nucl. States, Gatlinburg, Tenn., p.18, Abstr. B6 (1963)

E.Almqvist, J.A.Kuehner, D.McPherson, E.W.Vogt

Compound Nucleus Contributions to the C¹²(C¹², α)Ne²⁰ Reactions

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

1963EV03 Phys.Rev. 131, 818 (1963)

J.E.Evans, J.A.Kuehner, A.E.Litherland, E.Almqvist

Spin-Parity Combinations for Levels in Mg²⁴ and Si²⁸

NUCLEAR STRUCTURE ²⁸Si, ²⁴Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.131.818
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1963EV04 Phys.Rev. 131, 1632 (1963)

J.E.Evans, J.A.Kuehner, E.Almqvist

Study of the C¹²(d, p)C¹³ Reaction Mechanism; Polarization and (d, pγ) Correlations

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

doi: 10.1103/PhysRev.131.1632
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1963KU01 Bull.Am.Phys.Soc. 8, No.1, 25, F3 (1963)

J.A.Kuehner, J.D.Prentice, E.Almqvist

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

1963KU04 Phys.Canada 19, No.3, 14, Abstr.4.1 (1963)

J.A.Kuehner, J.D.Pearson

A New 5- Level in Ne²⁰

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

1963KU05 Phys.Letters 4, 332 (1963)

J.A.Kuehner, J.D.Prentice, E.Almqvist

High-Spin Resonances in C¹²(C¹², α)Ne²⁰

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

doi: 10.1016/0031-9163(63)90498-0
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1963KU12 Phys.Rev. 131, 1254 (1963)

J.A.Kuehner, E.Almqvist, D.A.Bromley

Elastic Scattering of Oxygen Ions by Carbon, Magnesium, and Aluminum

NUCLEAR STRUCTURE C, Al, Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.131.1254
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1962AL07 Phys.Can. 18, No.3, 40, 10.3 (1962)

E.Almqvist, J.E.Evans, J.A.Kuehner

Studies of the Polarization of Protons from (d, p) Stripping Reactions

NUCLEAR STRUCTURE ²⁹Si, ¹²C, ¹⁶O; measured not abstracted; deduced nuclear properties.

1962AL23 AECL-1659, p.11 (1962)

E.Almqvist, J.A.Kuehner, J.D.Prentice

Resonances in C¹²(C¹², α₀)Ne²⁰

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

1962EV01 Bull.Am.Phys.Soc. 7, No.1, 60, R12 (1962)

J.E.Evans, J.A.Kuehner, E.Almqvist

Polarization in the C¹²(d, p) Reaction

NUCLEAR STRUCTURE ¹²C, ¹³C; measured not abstracted; deduced nuclear properties.

1962EV02 AECL-1542, p.11 (1962)

J.E.Evans, J.A.Kuehner, E.Almqvist

Polarization Studies of C¹²(d, p)C^13*

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

1962EV04 Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 15, 5.9 (September 1962)

J.E.Evans, J.A.Kuehner, E.Almqvist

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

1962KU01 Bull.Am.Phys.Soc. 7, No.1, 73, V12 (1962)

J.A.Kuehner, A.E.Litherland, E.Almqvist, J.E.Evans

Parity Determinations for States of Mg²⁴ and Si²⁸

NUCLEAR STRUCTURE ²⁸Si, ²⁴Mg; measured not abstracted; deduced nuclear properties.

1962KU03 Phys.Rev. 125, 1650 (1962)

J.A.Kuehner

Spin and Parity Assignment to the 5.63-MeV and 5.80-MeV Levels of Ne²⁰

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

doi: 10.1103/PhysRev.125.1650
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1962KU04 Phys.Can. 18, No.3, 41, 10.4 (1962)

J.A.Kuehner, E.Almqvist

The Nuclear Surface as Determined by Heavy-Ion Elastic Scattering

1962KU05 AECL-1542, p.13 (1962)

J.A.Kuehner, E.Almqvist

Polarization in Si²⁸(d, p)Si²⁹

NUCLEAR STRUCTURE ²⁹Si; measured not abstracted; deduced nuclear properties.

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