NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = T.Engeland Found 52 matches. 2014EN03 Nucl.Phys. A928, 51 (2014) T.Engeland, M.Hjorth-Jensen, M.Kartamyshev, E.Osnes The Kuo-Brown effective interaction: From 18O to the Sn isotopes NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116Sn; calculated binding energy, mass excess, lowest 2+, 4+-state energy, B(E2). 101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131Sn; calculated single-particle levels, J, π. Large-scale shell model with different nucleon-nucleon potentials and effective interaction from G-matrix and Vlovk interactions. Compared with available data.
doi: 10.1016/j.nuclphysa.2014.03.012
2010EK01 Eur.Phys.J. A 44, 355 (2010) A.Ekstrom, J.Cederkall, C.Fahlander, M.Hjorth-Jensen, T.Engeland, A.Blazhev, P.A.Butler, T.Davinson, J.Eberth, F.Finke, A.Gorgen, M.Gorska, A.M.Hurst, O.Ivanov, J.Iwanicki, U.Koster, B.A.Marsh, J.Mierzejewski, P.Reiter, S.Siem, G.Sletten, I.Stefanescu, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, M.Zielinska Coulomb excitation of the odd-odd isotopes 106, 108In NUCLEAR REACTIONS 58Ni(106In, 106In'), (108In, 108In'), E=2.8 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation at the REX-ISOLDE facility. 106,108In; deduced levels, J, π, B(E2); calculated low-lying level properties, E2, M1 matrix elements using shell model plus coupled channels.
doi: 10.1140/epja/i2010-10945-7
2007KA40 Phys.Rev. C 76, 024313 (2007) M.P.Kartamyshev, T.Engeland, M.Hjorth-Jensen, E.Osnes Effective interactions and shell model studies of heavy tin isotopes NUCLEAR STRUCTURE 134,135,136,137,138,139,140,141,142Sn; calculated binding energies, single and two neutron separation energies, level energies, J, π, B(E2) using the single particle model.
doi: 10.1103/PhysRevC.76.024313
2006LE24 Phys.Rev. C 73, 064305 (2006) J.Leske, K.-H.Speidel, S.Schielke, J.Gerber, P.Maier-Komor, T.Engeland, M.Hjorth-Jensen Experimental g factor and B(E2) value of the 41+ state in Coulomb-excited 66Zn compared to shell-model predictions NUCLEAR REACTIONS C(66Zn, 66Zn'), E=180 MeV; measured Eγ, Iγ(θ, H, t), DSA, (recoil)γ-coin following projectile Coulomb excitation. 66Zn levels deduced T1/2, B(E2), g factors. Comparison with neighboring isotopes, shell-model calculations.
doi: 10.1103/PhysRevC.73.064305
2005BB09 Phys.Rev. C 72, 061305 (2005) A.Banu, J.Gerl, C.Fahlander, M.Gorska, H.Grawe, T.R.Saito, H.-J.Wollersheim, E.Caurier, T.Engeland, A.Gniady, M.Hjorth-Jensen, F.Nowacki, T.Beck, F.Becker, P.Bednarczyk, M.A.Bentley, A.Burger, F.Cristancho, G.de Angelis, Zs.Dombradi, P.Doornenbal, H.Geissel, J.Grebosz, G.Hammond, M.Hellstrom, J.Jolie, I.Kojouharov, N.Kurz, R.Lozeva, S.Mandal, N.Marginean, S.Muralithar, J.Nyberg, J.Pochodzalla, W.Prokopowicz, P.Reiter, D.Rudolph, C.Rusu, N.Saito, H.Schaffner, D.Sohler, H.Weick, C.Wheldon, M.Winkler 108Sn studied with intermediate-energy Coulomb excitation NUCLEAR REACTIONS 197Au(108Sn, 108Sn'), E=142 MeV; 197Au(112Sn, 112Sn'), E=147 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 108,112Sn levels deduced excitation B(E2), core polarization features. Comparison with large-scale shell model predictions.
doi: 10.1103/PhysRevC.72.061305
2005EL05 Phys.Rev. C 71, 034301 (2005) P.J.Ellis, T.Engeland, M.Hjorth-Jensen, M.P.Kartamyshev, E.Osnes Model calculation of effective three-body forces
doi: 10.1103/PhysRevC.71.034301
2005LE38 Phys.Rev. C 72, 044301 (2005) J.Leske, K.-H.Speidel, S.Schielke, J.Gerber, P.Maier-Komor, T.Engeland, M.Hjorth-Jensen Dominant (g9/2)2 neutron configuration in the 4+1 state of 68Zn based on new g factor measurements NUCLEAR REACTIONS C(68Zn, 68Zn'), E=180 MeV; measured Eγ, Iγ(θ, H, t) (particle)γ-coin following projectile Coulomb excitation. 68Zn levels deduced g factors, T1/2, B(E2), configurations. 64Zn levels analyzed g factors, B(E2). Large-scale shell-model calculations.
doi: 10.1103/PhysRevC.72.044301
2004DE35 Prog.Part.Nucl.Phys. 53, 419 (2004) D.J.Dean, T.Engeland, M.Hjorth-Jensen, M.P.Kartamyshev, E.Osnes Effective interactions and the nuclear shell-model
doi: 10.1016/j.ppnp.2004.05.001
2004GA24 Phys.Rev. C 69, 054307 (2004) H.Gausemel, B.Fogelberg, T.Engeland, M.Hjorth-Jensen, P.Hoff, H.Mach, K.A.Mezilev, J.P.Omtvedt Decay of 127In and 129In RADIOACTIVITY 127,129In(β-) [from 235U(n, F)]; measured Eβ, Eγ, γγ-, βγ-coin following ground-state and isomer decays. 127,129In deduced isomeric states energies, T1/2. 127,129Sn deduced levels, J, π, isomers T1/2. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.69.054307
2002EN07 Nucl.Phys. A701, 416c (2002) T.Engeland, M.Hjorth-Jensen, E.Osnes Effective Interactions in Medium Heavy Nuclei NUCLEAR STRUCTURE 116,118,120,122,124,126,128,130Sn, 105,106,107Sb; calculated levels, J, π. Shell model, realistic effective interactions, comparison with data.
doi: 10.1016/S0375-9474(01)01620-7
2002LI04 Phys.Rev. C65, 021302 (2002) M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu 100Sn Core Excitations in 102In NUCLEAR REACTIONS 50Cr(58Ni, npα), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 102In deduced levels, possible J, π, configurations. Gammasphere, Microball arrays. Comparison with large-scale shell model calculations.
doi: 10.1103/PhysRevC.65.021302
2002LI33 Phys.Rev. C65, 051307 (2002) M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.H.Yu Excited States of the Proton Emitter 105Sb NUCLEAR REACTIONS 50Cr(58Ni, 2np), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 105Sb deduced levels, possible J, π. Gammasphere, Microball arrays. Comparison with shell model results.
doi: 10.1103/PhysRevC.65.051307
2002LI45 Phys.Rev. C66, 011302 (2002) M.Lipoglavsek, C.Baktash, J.Blomqvist, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu Breakup of the Doubly Magic 100Sn Core NUCLEAR REACTIONS 50Cr(58Ni, xnypzα)99Cd/101In, E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin; deduced relative yields. 99Cd, 101In deduced high-spin levels, J, π, configurations, core excitation. Gammasphere, Microball arrays, large-scale shell model calculations.
doi: 10.1103/PhysRevC.66.011302
2000EN02 Phys.Rev. C61, 021302 (2000) T.Engeland, M.Hjorth-Jensen, E.Osnes Shell-Model Studies of the Proton Drip Line Nucleus 106Sb NUCLEAR STRUCTURE 106Sb; calculated levels, J, π, B(E2). Shell model, comparison with data.
doi: 10.1103/PhysRevC.61.021302
2000HO15 Phys.Rev. C61, 064318 (2000) A.Holt, T.Engeland, M.Hjorth-Jensen, E.Osnes Application of Realistic Effective Interactions to the Structure of the Zr Isotopes NUCLEAR STRUCTURE 90,91,92,93,94,95,96,97,98Zr; calculated levels, J, π, configurations, B(E2). Shell model, realistic effective interactions, comparisons with data.
doi: 10.1103/PhysRevC.61.064318
1998HO11 Nucl.Phys. A634, 41 (1998) A.Holt, T.Engeland, M.Hjorth-Jensen, E.Osnes Effective Interactions and Shell Model Studies of Heavy Tin Isotopes NUCLEAR STRUCTURE 120,121,122,123,124,125,126,127,128,129,130Sn; calculated levels, J, π, B(E2); deduced effective interaction features. Shell model, perturbative many-body technique.
doi: 10.1016/S0375-9474(98)00146-8
1998SU03 Nucl.Phys. A628, 41 (1998) J.Suhonen, J.Toivanen, A.Holt, T.Engeland, E.Osnes, M.Hjorth-Jensen Study of Odd-Mass N = 82 Isotones with Realistic Effective Interactions NUCLEAR STRUCTURE 135I, 137Cs, 139La, 141Pr, 143Pm, 145Eu; calculated levels, J, π. Microscopic quasiparticle-phonon model, realistic G-matrix-based effective interactions.
doi: 10.1016/S0375-9474(97)00615-5
1997HO05 Nucl.Phys. A618, 107 (1997) A.Holt, T.Engeland, E.Osnes, M.Hjorth-Jensen, J.Suhonen Extended Shell Model Calculation for Even N = 82 Isotones with a Realistic Effective Interaction NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm; calculated levels, B(λ), proton occupation numbers, other aspects. Extended shell model.
doi: 10.1016/S0375-9474(97)00123-1
1997SA22 Phys.Rev. C55, 2708 (1997) N.Sandulescu, J.Blomqvist, T.Engeland, M.Hjorth-Jensen, A.Holt, R.J.Liotta, E.Osnes Generalized Seniority Scheme in Light Sn Isotopes NUCLEAR STRUCTURE 104,106,108,110,112Sn; calculated levels, wave functions. Generalized seniority scheme, shell model, truncation.
doi: 10.1103/PhysRevC.55.2708
1995EN05 Phys.Scr. T56, 58 (1995) T.Engeland, M.Hjorth-Jensen, A.Holt, E.Osnes Large Shell Model Calculations with Realistic Effective Interaction NUCLEAR STRUCTURE 102,103,104,105,106,107,108,109,110,111,112Sn; calculated levels. Large basis shell model.
doi: 10.1088/0031-8949/1995/T56/009
1994EL07 Nucl.Phys. A573, 216 (1994) P.J.Ellis, T.Engeland, M.Hjorth-Jensen, A.Holt, E.Osnes Convergence Properties of the Effective Interaction NUCLEAR STRUCTURE 18O; calculated level energy vs starting energy. Folded diagram, Lee-Suzuki models comparison.
doi: 10.1016/0375-9474(94)90168-6
1994HO07 Nucl.Phys. A570, 137c (1994) A.Holt, T.Engeland, M.Hjorth-Jensen, E.Osnes The Structure of Neutron Deficient Sn Isotopes NUCLEAR STRUCTURE 102,104,106,108,110,112,105,107Sn; calculated levels. Shell model, effective interaction.
doi: 10.1016/0375-9474(94)90277-1
1993EN02 Phys.Rev. C48, R535 (1993) T.Engeland, M.Hjorth-Jensen, A.Holt, E.Osnes Structure of Neutron Deficient Sn Isotopes NUCLEAR STRUCTURE 102,104,106Sn; calculated levels, B(λ). Shell model.
doi: 10.1103/PhysRevC.48.R535
1992HJ03 Nucl.Phys. A541, 105 (1992) M.Hjorth-Jensen, T.Engeland, A.Holt, E.Osnes On the Role of Third- and Higher-Order Contributions to the Effective Interaction for pf Shell Nuclei NUCLEAR STRUCTURE 44Ca, 44Sc, 44Ti; calculated level relative to 40Ca. Effective interaction, third-, higher-order contributions in perturbation theory, Bonn, Paris potentials based meson-exchange interaction.
doi: 10.1016/0375-9474(92)90636-X
1987RA16 Nucl.Phys. A470, 79 (1987) T.Ramsoy, A.Atac, T.Engeland, M.Guttormsen, J.Rekstad, G.Lovhoiden, T.F.Thorsteinsen, J.S.Vaagen Particle-Vibration Coupled States in 161Dy NUCLEAR REACTIONS 161Dy(3He, 3He'), E=32 MeV; measured σ(E), Eγ, Iγ, 3Heγ-coin. 161Dy deduced levels, J, π. Particle-core model calculations. Ge, Si counters, enriched target.
doi: 10.1016/0375-9474(87)90121-7
1986EN07 Phys.Scr. 34, 703 (1986) Population of Non-Coherent Intrinsic States in Anomalous (t, p) Monopole Transfer on Odd-Mass Rare-Earth Isotopes NUCLEAR STRUCTURE 181Hf, 169Er, 163Dy; calculated levels, pair occupation amplitudes, pair gaps, (t, p) transfer strengths. Microscopic model.
doi: 10.1088/0031-8949/34/6A/027
1983AA01 Phys.Rev. C28, 1857 (1983) R.M.Aasen, J.Rekstad, A.Henriquez, F.Ingebretsen, M.Guttormsen, T.Engeland Gamma-Ray Energy Dependence of Transition Probabilities in the Continuum NUCLEAR REACTIONS 149Sm(3He, α), E=26 MeV; measured σ(E(α)), γα-coin. 148Sm deduced γ-ray multiplicity. Enriched target, Ge(Li), NaI(Tl), Si detectors. Fermi gas model analysis.
doi: 10.1103/PhysRevC.28.1857
1983EN01 Phys.Lett. 120B, 19 (1983) T.Engeland, A.Henriquez, J.Rekstad The Coriolis Attenuation Problem in the Perturbed i13/2 Neutron Bands NUCLEAR STRUCTURE 151Sm, 153Gd, 163Er, 181W; calculated levels, quasiparticle energies, Coriolis attentuation factors; deduced Coriolis coupling BCS approximation dependence. Pairing plus recoil model.
doi: 10.1016/0370-2693(83)90613-5
1983HE03 Phys.Rev. C27, 1302 (1983) A.Henriquez, T.Engeland, J.Rekstad Particle-Rotor Model Calculation of 109Pd NUCLEAR STRUCTURE 109Pd; calculated levels. Particle-rotor model, no Coriolis attennuation.
doi: 10.1103/PhysRevC.27.1302
1983HE22 Nucl.Phys. A410, 1 (1983) A.Henriquez, T.Engeland, J.Rekstad The Coriolis Attenuation Problem in 235U NUCLEAR STRUCTURE 235U; calculated levels, B(E2). Particle-rotor model, Coriolis attenuation.
doi: 10.1016/0375-9474(83)90397-4
1983RE09 Phys.Scr. T5, 45 (1983) J.Rekstad, A.Henriquez, F.Ingebretsen, G.Midttun, B.Skaali, R.Oyan, J.Wikne, T.Engeland, T.G.Thorsteinsen, E.Hammaren, E.Liukkonen A Study of the Nuclear Structure at High Energy and Low Spin NUCLEAR REACTIONS 147,149Sm, 155,157Gd, 161,163Dy(3He, α), E=26 MeV; measured Eα, Iα, γα-coin, γ-multiplicity spectra; deduced structure change in deformed nuclei. 146,148Sm, 156Gd, 160,162Dy deduced < Eγ > vs excitation energy. 154Gd deduced < Eγ > vs excitation energy, γ-transition relative intensities.
doi: 10.1088/0031-8949/1983/T5/007
1982EN02 Phys.Scr. 25, 467 (1982) The Particle-Rotor Model and the Coriolis Attenuation Problem in 163Er NUCLEAR STRUCTURE 163Er; calculated levels; deduced rotational band characteristics. Particle-rotor model.
doi: 10.1088/0031-8949/25/3/006
1981RE11 Nucl.Phys. A371, 364 (1981) J.Rekstad, P.Boe, A.Henriquez, R.Oyan, M.Guttormsen, T.Engeland, G.Lovhoiden The Level Structure of the 153Gd Nucleus Studied in the 150Sm(α, n)153Gd Reaction NUCLEAR REACTIONS 150Sm(α, n), E=17, 19 MeV; measured Eγ, Iγ, γγ-coin, γ-multiplicities. 153Gd deduced levels, J, π, K. Enriched target, Ge(Li), NaI detectors.
doi: 10.1016/0375-9474(81)90052-X
1980GU07 Nucl.Phys. A338, 141 (1980) M.Guttormsen, T.Pedersen, J.Rekstad, T.Engeland, E.Osnes, F.Ingebretsen The Particle-Rotor Model with Pairing in the s-d Shell. An Analysis Of the 23Na Nucleus NUCLEAR STRUCTURE 23Na; calculated stripping, pickup S, levels, T1/2, B(λ). Particle-rotor model, pairing effects.
doi: 10.1016/0375-9474(80)90126-8
1979RE04 Nucl.Phys. A320, 239 (1979) J.Rekstad, M.Guttormsen, T.Engeland, G.Lovhoiden, O.Straume, J.Lien, C.E.Ellegaard The 153Sm Nucleus: An Experimental and Theoretical Study NUCLEAR REACTIONS 150Nd(α, n), E=14-22 MeV; measured Eγ, Iγ, γγ-coin. 153Sm deduced levels, J, π, K. Enriched target. Ge(Li) detectors.
doi: 10.1016/0375-9474(79)90187-8
1979RE10 Nucl.Phys. A330, 367 (1979) J.Rekstad, T.Engeland, E.Osnes Evidence for the Two-body Nature of the Recoil Term in the Particle-Rotor Model NUCLEAR STRUCTURE 150,151,152,153,154,155,156,157,158,159,160Gd, 64,65,66,67,68,69,70,71Zn, 70,71,72,73,74,75,76,77Ge; calculated recoil energy. Particle-rotor model, two-body part of recoil term.
doi: 10.1016/0375-9474(79)90060-5
1977PE23 Nucl.Phys. A293, 10 (1977) T.Pedersen, T.Engeland, I.Espe, J.Rekstad, C.Ellegaard, S.Backe A Study of 15N by Use of the Reaction 13C(3He, p)15N NUCLEAR REACTIONS 13C(3He, 3He), E=20 MeV; measured σ(E(3He), θ). 13C(3He, p), E=20 MeV; measured σ(Ep, θ). 15N levels deduced structure. Enriched target.
doi: 10.1016/0375-9474(77)90473-0
1976EN01 Phys.Lett. 60B, 321 (1976) T.Engeland, E.Osnes, D.Strottman Nuclear Structure Aspects of the g-Factor of the 3.83 MeV (15/2+) Level in 41Ca NUCLEAR STRUCTURE 41Ca level; calculated g.
doi: 10.1016/0370-2693(76)90739-5
1976EN03 Phys.Rev.Lett. 36, 994 (1976) Comment on the Quadrupole Moment of the First-Excited 2+ State of 18O NUCLEAR MOMENTS 18O; analyzed data on first 2+ level quadrupole moment.
doi: 10.1103/PhysRevLett.36.994
1976FI01 Nucl.Phys. A258, 317 (1976) M.A.Firestone, J.Janecke, A.Dudek-Ellis, P.J.Ellis, T.Engeland The 16O(d, 3He)15N Reaction at 29 Mev: Reaction Mechanism and Nuclear Structure NUCLEAR REACTIONS 16O(d, 3He), E=29 MeV; measured σ(E(3He), θ). 15N deduced levels, J, π, S. Coupled channels, DWBA analysis.
doi: 10.1016/0375-9474(76)90009-9
1976LI16 Nucl.Phys. A267, 123 (1976) The A = 15 Nuclei in the Weak Coupling Model NUCLEAR STRUCTURE 15N, 15O, 15C; calculated levels, Γ.
doi: 10.1016/0375-9474(76)90647-3
1974AN36 Phys.Rep. 12, 201 (1974) N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 11B), (12C, 11C), (12C, 10B), (12C, 10Be), (12C, 10C), (12C, 9Be), E=114 MeV; 12,13C(11B, 9Li), E=114 MeV; 13C(11B, 10B), E=114 MeV; measured particle spectra, σ(E, θ). 13,14C, 13,14,15N, 14,15O deduced levels, J, π, spectroscopic amplitudes.
doi: 10.1016/0370-1573(74)90045-3
1974EN03 Nucl.Phys. A226, 45 (1974) Nuclear Structure Calculation of 50Sc and Analysis of the 48Ca(3He, p)50Sc Reaction NUCLEAR STRUCTURE 50Sc; calculated levels. NUCLEAR REACTIONS 48Ca(3He, p); calculated reaction strength.
doi: 10.1016/0375-9474(74)90599-5
1973RE10 Phys.Lett. 45B, 77 (1973) A Study of Photoproduction of Charged Pions from 16O NUCLEAR REACTIONS 16O(γ, π+); measured nothing, calculated σ(E). 16N deduced levels, J, π.
doi: 10.1016/0370-2693(73)90068-3
1972EN03 Nucl.Phys. A181, 368 (1972) The Weak Coupling Model Applied to the Nuclei with A = 16-19. (II). Gamma Transitions and Spectroscopic Factors NUCLEAR STRUCTURE 16O, 17O, 18O, 17,18,19F, 18,19Ne; calculated γ-transition rates, level-width, S, B(λ). Weak coupling model.
doi: 10.1016/0375-9474(72)90490-3
1971LI17 Nucl.Phys. A169, 617 (1971) An Application of the Weak Coupling Model to the Negative-Parity States of the A=15 Nuclei NUCLEAR STRUCTURE 15N, 15O; calculated levels, level-width, wave functions, branching ratios. Weak coupling model.
doi: 10.1016/0375-9474(71)90706-8
1970EL23 Nucl.Phys. A144, 161 (1970) The weak coupling model applied to the nuclei with A = 16–19: (I). Energy levels NUCLEAR STRUCTURE 16,17,18O, 18,19F; calculated energy levels, J, π; deduced particle-hole states by coupling in J and T eigenfunctions resulting from diagonalization of (sd)n1 and pn2, positive parity levels.
doi: 10.1016/0375-9474(70)90499-9
1970LI23 Nucl.Phys. A156, 449 (1970) A Weak Coupling Calculation for the Positive Parity States of the A = 15 Nuclei NUCLEAR STRUCTURE 15N, 15O; calculated positive-parity states.
doi: 10.1016/0375-9474(70)90243-5
1967EN01 Phys.Letters 25B, 57 (1967) Calculation of Particle-Hole States in the 2s-1d Shell
doi: 10.1016/0370-2693(67)90175-X
1967WA03 Nucl.Phys. A94, 129 (1967) Shell-Model Calculation in 24Mg NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(67)90813-5
1966EN01 Phys.Letters 20, 424 (1966) Shell Model Calculations in the Calcium-Isotopes NUCLEAR STRUCTURE 44Ca, 43Ca, 42Ca, 47Ca, 46Ca, 45Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90769-4
1965EN02 Nucl.Phys. 72, 68 (1965) Core Excitation in O18 NUCLEAR STRUCTURE 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90627-9
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