NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Kuehner Found 143 matches. Showing 1 to 100. [Next]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
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
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
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
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
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. 145,146,147,148,149Gd 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
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
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 T1/2, B(M1).
doi: 10.1016/0375-9474(91)90293-F
1990HA31 Phys.Rev. C42, R1817 (1990) B.Haas, D.Ward, H.R.Andrews, G.C.Ball, T.E.Drake, S.Flibotte, A.Galindo-Uribarri, V.P.Janzen, J.K.Johansson, H.Kluge, J.Kuehner, A.Omar, S.Pilotte, D.Prevost, J.Rodriguez, D.C.Radford, P.Taras, J.P.Vivien, J.C.Waddington, S.Aberg Observation of Excited Proton and Neutron Configurations in the Superdeformed 149Gd Nucleus NUCLEAR REACTIONS 124Sn(30Si, 5n), E=155 MeV; 124Sn(31P, 5n), E=156 MeV; measured γ-spectra, γγ-coin. 149Gd deduced levels, J, π, superdeformed band structure.
doi: 10.1103/PhysRevC.42.R1817
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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 124,126,128,130Te(t, d), E=16 MeV; measured σ(Ed, θ). 125,127,129,131Te levels deduced L, S, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.23.64
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
1981WA03 Nucl.Phys. A356, 33 (1981) A.Warwick, R.Chapman, J.L.Durell, J.N.Mo, J.A.Kuehner, P.Skensved The 1h9/2 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 1h9/2 proton wave function. Zero-range, finite-range DWBA analysis.
doi: 10.1016/0375-9474(81)90116-0
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 3p1/2 neutron orbit rms radius. DWBA analysis.
doi: 10.1016/0370-2693(81)90775-9
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
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
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 124,126,128,130Te(t, α), E=16 MeV; measured σ(Eα, θ). 123,125,127,129Sb levels deduced C2S. DWBA.
doi: 10.1103/PhysRevC.21.1116
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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, T1/2.
doi: 10.1103/PhysRevC.12.887
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
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
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
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
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, T1/2, λ, B(E2).
doi: 10.1103/PhysRevC.12.468
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, T1/2, γ-branching ratios, γ-mixing.
doi: 10.1139/p74-130
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, T1/2, γ-branching ratios, λ.
doi: 10.1139/p74-195
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, T1/2, J, π.
doi: 10.1139/p73-154
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, T1/2, γ-branching.
doi: 10.1103/PhysRevLett.28.571
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 T1/2. Natural target.
doi: 10.1016/0375-9474(72)90183-2
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
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
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
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
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
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
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
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, T1/2, γ-branching. Ge(Li) detector.
doi: 10.1139/p69-085
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, T1/2.
doi: 10.1139/p69-282
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
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
1967KU04 Can.J.Phys. 45, 1605 (1967) New High-Spin Levels in 20Ne NUCLEAR STRUCTURE 12C, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p67-124
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
1966KU03 Phys.Letters 20, 301 (1966) 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
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
1965KU01 Bull.Am.Phys.Soc. 10, No.1, 37, CC8 (1965) 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) 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
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
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
1964KU03 Can.J.Phys. 42, 477 (1964) New 5- and 6+ States in Ne20 NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p64-043
1964KU04 Bull.Am.Phys.Soc. 9, No.4, 430, EA9 (1964); Priv.Comm. (1964) 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
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
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
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
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
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) 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
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
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)C13* 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) 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
1962KU04 Phys.Can. 18, No.3, 41, 10.4 (1962) The Nuclear Surface as Determined by Heavy-Ion Elastic Scattering
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