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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1986EN07      Phys.Scr. 34, 703 (1986)

T.Engeland, J.S.Vaagen

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
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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
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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
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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
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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
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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
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1982EN02      Phys.Scr. 25, 467 (1982)

T.Engeland

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1298.


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
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1976EN03      Phys.Rev.Lett. 36, 994 (1976)

T.Engeland, P.J.Ellis

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
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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
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1976LI16      Nucl.Phys. A267, 123 (1976)

S.Lie, T.Engeland

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
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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
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1974EN03      Nucl.Phys. A226, 45 (1974)

T.Engeland, E.Osnes

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
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1973RE10      Phys.Lett. 45B, 77 (1973)

A.K.Rej, T.Engeland

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
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1972EN03      Nucl.Phys. A181, 368 (1972)

T.Engeland, P.J.Ellis

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
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1971LI17      Nucl.Phys. A169, 617 (1971)

S.Lie, T.Engeland

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
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1970EL23      Nucl.Phys. A144, 161 (1970)

P.J.Ellis, T.Engeland

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
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1970LI23      Nucl.Phys. A156, 449 (1970)

S.Lie, T.Engeland, G.Dahll

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
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1967EN01      Phys.Letters 25B, 57 (1967)

T.Engeland, P.J.Ellis

Calculation of Particle-Hole States in the 2s-1d Shell

doi: 10.1016/0370-2693(67)90175-X
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1967WA03      Nucl.Phys. A94, 129 (1967)

K.Wathne, T.Engeland

Shell-Model Calculation in 24Mg

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

doi: 10.1016/0375-9474(67)90813-5
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1966EN01      Phys.Letters 20, 424 (1966)

T.Engeland, E.Osnes

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
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1965EN02      Nucl.Phys. 72, 68 (1965)

T.Engeland

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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