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NSR database version of April 27, 2024.

Search: Author = E.Osnes

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2017KU03      Int.J.Mod.Phys. E26, 1740013 (2017)

T.T.S.Kuo, T.K.Kuo, E.Osnes, S.Shu

Nucleon-anti-nucleon intruder state of Dirac equation for nucleon in deep scalar potential well

NUCLEAR STRUCTURE ¹⁸O; calculated energy levels, J, π. Comparison with available data.

doi: 10.1142/S0218301317400134
Citations: PlumX Metrics

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 ^{102,104,106,108,110,112,114,116}Sn; calculated binding energy, mass excess, lowest 2⁺, 4⁺-state energy, B(E2). ^{101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131}Sn; calculated single-particle levels, J, π. Large-scale shell model with different nucleon-nucleon potentials and effective interaction from G-matrix and V_lovk interactions. Compared with available data.

doi: 10.1016/j.nuclphysa.2014.03.012
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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 ^{134,135,136,137,138,139,140,141,142}Sn; 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
Citations: PlumX Metrics

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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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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2002EN07      Nucl.Phys. A701, 416c (2002)

T.Engeland, M.Hjorth-Jensen, E.Osnes

Effective Interactions in Medium Heavy Nuclei

NUCLEAR STRUCTURE ^{116,118,120,122,124,126,128,130}Sn, ^105,106,107Sb; calculated levels, J, π. Shell model, realistic effective interactions, comparison with data.

doi: 10.1016/S0375-9474(01)01620-7
Citations: PlumX Metrics

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 ^{90,91,92,93,94,95,96,97,98}Zr; 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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1998EL03      Phys.Rev. C57, R1069 (1998)

O.Elgaroy, L.Engvik, M.Hjorth-Jensen, E.Osnes

Minimal Relativity and ³S₁-³D₁ Pairing in Symmetric Nuclear Matter

doi: 10.1103/PhysRevC.57.R1069
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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 ^{120,121,122,123,124,125,126,127,128,129,130}Sn; 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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1997EN04      Nucl.Phys. A622, 553 (1997)

L.Engvik, E.Osnes, M.Hjorth-Jensen, T.T.S.Kuo

Nuclear and Neutron Matter Calculations with Different Model Spaces

doi: 10.1016/S0375-9474(97)00359-X
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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 ^{104,106,108,110,112}Sn; calculated levels, wave functions. Generalized seniority scheme, shell model, truncation.

doi: 10.1103/PhysRevC.55.2708
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1996EL07      Nucl.Phys. A604, 466 (1996)

O.Elgaroy, L.Engvik, M.Hjorth-Jensen, E.Osnes

Model-Space Approach to ¹S₀ Neutron and Proton Pairing in Neutron Star Matter with the Bonn Meson-Exchange Potentials

doi: 10.1016/0375-9474(96)00152-2
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1996EL09      Nucl.Phys. A607, 425 (1996)

O.Elgaroy, L.Engvik, M.Hjorth-Jensen, E.Osnes

Triplet Pairing of Neutrons in β-Stable Neutron Star Matter

doi: 10.1016/S0375-9474(96)00217-5
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1996HJ02      J.Phys.(London) G22, 321 (1996)

M.Hjorth-Jensen, H.Muther, E.Osnes, A.Polls

Comparison of the Effective Interaction to Various Orders in Different Mass Regions

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ⁴⁰Ca, ¹⁰⁰Sn, ²⁰⁸Pb; calculated diagonal, nondiagonal matrix elements, mean value ratios; deduced higher-order terms contributions stability mass dependence. Effective interaction to various orders, shell model.

doi: 10.1088/0954-3899/22/3/006
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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 ^{102,103,104,105,106,107,108,109,110,111,112}Sn; calculated levels. Large basis shell model.

doi: 10.1088/0031-8949/1995/T56/009
Citations: PlumX Metrics

1995HJ01      Phys.Rep. 261, 125 (1995)

M.Hjorth-Jensen, T.T.S.Kuo, E.Osnes

Realistic Effective Interactions for Nuclear Systems

doi: 10.1016/0370-1573(95)00012-6
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1994BA47      Nucl.Phys. A575, 707 (1994)

G.Bao, L.Engvik, M.Hjorth-Jensen, E.Osnes, E.Ostgaard

Neutron-Star Properties from Modern Meson-Exchange Potential Models

doi: 10.1016/0375-9474(94)90163-5
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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
Citations: PlumX Metrics

1994HO07      Nucl.Phys. A570, 137c (1994)

A.Holt, T.Engeland, M.Hjorth-Jensen, E.Osnes

The Structure of Neutron Deficient Sn Isotopes

NUCLEAR STRUCTURE ^{102,104,106,108,110,112,105,107}Sn; calculated levels. Shell model, effective interaction.

doi: 10.1016/0375-9474(94)90277-1
Citations: PlumX Metrics

1994TZ01      Nucl.Phys. A580, 277 (1994)

S.Y.T.Tzeng, P.J.Ellis, T.T.S.Kuo, E.Osnes

Finite-Temperature Many-Body Theory with the Lipkin Model

doi: 10.1016/0375-9474(94)90774-9
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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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1992HJ01      Ann.Phys.(New York) 213, 102 (1992)

M.Hjorth-Jensen, E.Osnes, H.Muther

Folded-Diagram Effective Interactions with the Bonn Meson-Exchange Potential Model

NUCLEAR STRUCTURE ¹⁸O, ²⁰Ne; calculated levels. Bonn meson-exchange potential model, folded-diagram effective interactions, Brueckner-Hartree-Fock basis.

doi: 10.1016/0003-4916(92)90285-T
Citations: PlumX Metrics

1992HJ02      Nucl.Phys. A540, 145 (1992)

M.Hjorth-Jensen, E.Osnes, T.T.S.Kuo

Effective Interactions for Valence-Hole Nuclei with Modern Meson-Exchange Potential Models

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated single particle energies. A=14, 38; calculated degenerate, nondegenerate unperturbed single particle energies. Folded diagram theory, effective interaction.

doi: 10.1016/0375-9474(92)90198-S
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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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1992OS01      Phys.Rev. C45, 662 (1992)

E.Osnes, D.Strottman

Spin-Tensor Analysis of Realistic Shell Model Interactions

NUCLEAR STRUCTURE ¹⁸O; calculated levels. Realistic shell model interactions, spin-tensor analysis.

doi: 10.1103/PhysRevC.45.662
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1990HJ01      Phys.Scr. 41, 207 (1990)

M.Hjorth-Jensen, E.Osnes

Number-Conserving Sets and Effective Interactions through Third Order for Mass-18 with the Bonn-Julich Potential

NUCLEAR STRUCTURE A=18; calculated T=0, 1 spectra. Number conserving sets, effective interactions, Bonn-Julich potential.

doi: 10.1088/0031-8949/41/2/004
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1990HJ03      Phys.Lett. 248B, 243 (1990)

M.Hjorth-Jensen, E.Osnes, H.Muther, K.W.Schmid

Choice of Single-Particle Potential and the Convergence of the Effective Interaction

NUCLEAR STRUCTURE ¹⁸O, ¹⁸F; calculated levels; deduced effective interaction convergence. Harmonic oscillator, Brueckner-Hartree-Fock basis.

doi: 10.1016/0370-2693(90)90285-E
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1989HJ03      Phys.Lett. 228B, 281 (1989)

M.Hjorth-Jensen, E.Osnes

Effective Interactions through Third Order for Mass-18 Nuclei with the Paris Potential

NUCLEAR STRUCTURE ¹⁸F, ¹⁸O; calculated levels; deduced effective interaction dependence.

doi: 10.1016/0370-2693(89)91545-1
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1983PO02      Nucl.Phys. A401, 124 (1983)

A.Polls, H.Muther, A.Faessler, T.T.S.Kuo, E.Osnes

Three-Body Forces in sd-Shell Nuclei

NUCLEAR STRUCTURE A=19; calculated T=1/2 levels. ¹⁹O; calculated T=3/2 levels. Three-body forces, shell model.

doi: 10.1016/0375-9474(83)90340-8
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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, T_1/2, B(λ). Particle-rotor model, pairing effects.

doi: 10.1016/0375-9474(80)90126-8
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1980KU05      J.Phys.(London) G6, 335 (1980)

T.T.S.Kuo, E.Osnes

Calculation of E2 Transition Rates in A = 18-19 Nuclei with Realistic Effective Interaction and Charges

NUCLEAR STRUCTURE ^18,19O, ^18,19F; calculated levels, B(E2). Shell model, realistic effective interaction, screened Tamm-Dancoff approximation charges.

doi: 10.1088/0305-4616/6/3/009
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1979PE16      Nucl.Phys. A332, 1 (1979)

T.Pedersen, E.Osnes, M.Guttormsen

The Kπ = 1/2^- Bands in the Odd-A = 19-31 Nuclei

NUCLEAR STRUCTURE A=19-31; calculated level energies, S, B(λ). Nilsson orbits, weak-coupling, particle-rotor models.

doi: 10.1016/0375-9474(79)90090-3
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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 ^{150,151,152,153,154,155,156,157,158,159,160}Gd, ^{64,65,66,67,68,69,70,71}Zn, ^{70,71,72,73,74,75,76,77}Ge; calculated recoil energy. Particle-rotor model, two-body part of recoil term.

doi: 10.1016/0375-9474(79)90060-5
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1978GU11      Nucl.Phys. A298, 122 (1978)

M.Guttormsen, E.Osnes, J.Rekstad, G.Lovhoiden, O.Straume

Particle-Rotor Model Description of the Negative-Parity States in the Transitional ¹⁵¹Sm Nucleus

NUCLEAR STRUCTURE ¹⁵¹Sm; calculated levels, B(λ), S.

doi: 10.1016/0375-9474(78)90011-8
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1978PE09      Nucl.Phys. A303, 345 (1978)

T.Pedersen, E.Osnes

Decoupled Bands and Antialigned States: An Illustrative Example

NUCLEAR STRUCTURE ¹⁹F, ²³Ne; calculated levels, bands.

doi: 10.1016/0375-9474(78)90363-9
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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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1976RE06      Phys.Lett. 62B, 15 (1976)

J.Rekstad, E.Osnes, G.Lovhoiden

Rotational Description of the Negative-Parity States in Transitional N = 89 Nuclei

NUCLEAR STRUCTURE ¹⁵¹Sm, ¹⁵³Gd; calculated level energies, pick-up S for low-spin negative-parity states.

doi: 10.1016/0370-2693(76)90035-6
Citations: PlumX Metrics

1975BA37      Nucl.Phys. A248, 429 (1975)

B.R.Barrett, W.-T.Weng, E.Osnes, J.Richert

Model Calculations for ⁵⁰Ca and the Convergence Properties of the Perturbation Expansion for the Effective Interaction

NUCLEAR STRUCTURE ⁵⁰Ca; calculated convergence properties of different perturbation schemes for computing effective interaction.

doi: 10.1016/0375-9474(75)90522-9
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1975KU16      Phys.Rev. C12, 309 (1975)

T.T.S.Kuo, E.Osnes

Calculation of B(E2) Transition Rates in 1f₇/₂-Shell Nuclei with Realistic Effective Interaction and Charges

NUCLEAR STRUCTURE ^42,43Ca, ^42,43Sc; calculated B(E2).

doi: 10.1103/PhysRevC.12.309
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1975OL04      Phys.Norv. 8, 85 (1975)

T.H.Olsen, E.Osnes

Shell-Model Study of the Nuclear A = 43 System

NUCLEAR STRUCTURE ⁴³Sc, ⁴³Ca; calculated levels, level properties. Shell model.

1974EL01      Phys.Lett. 49B, 23 (1974)

P.J.Ellis, E.Osnes

Monopole Core Polarization in a Hartree-Fock Basis

NUCLEAR STRUCTURE ¹⁶O; calculated particle-hole states, monopole core polarization.

doi: 10.1016/0370-2693(74)90571-1
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1974EL05      Phys.Lett. 52B, 31 (1974)

P.J.Ellis, E.Osnes

On Possible Collective Effects in the Positive Parity Particle-Hole States of ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated levels.

doi: 10.1016/0370-2693(74)90710-2
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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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1974HA60      Phys.Lett. 53B, 129 (1974)

I.Hamamoto, E.Osnes

Simple Two-Level Model of the Hole-Vibration Quadruplet in ³⁹K

NUCLEAR STRUCTURE ³⁹K; calculated levels, E3 strengths.

doi: 10.1016/0370-2693(74)90511-5
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1974KU08      Nucl.Phys. A226, 204 (1974)

T.T.S.Kuo, E.Osnes

Self-Screening of the Particle-Hole Interaction and Core Polarization of the Effective Two-Particle Interaction

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated monopole states.

doi: 10.1016/0375-9474(74)90402-3
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1973KU04      Nucl.Phys. A205, 1 (1973)

T.T.S.Kuo, E.Osnes

Self-Screening of the Particle-Hole Interaction and the Effective Charge

NUCLEAR STRUCTURE A=17, A=41; calculated polarization charges. ¹⁶O, ⁴⁰Ca calculated isoscalar quadrupole resonance.

doi: 10.1016/0375-9474(73)90115-2
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1973OS02      Phys.Lett. 47B, 430 (1973)

E.Osnes, T.T.S.Kuo

The T = 1 to T = 0 Splitting of the f₇/₂d^-1₃/₂ Particle-Hole Multiplet

NUCLEAR STRUCTURE ³⁸Cl, ⁴⁰K, ⁴⁰Ca; levels calculated J-dependence of T=0, 1 splitting.

doi: 10.1016/0370-2693(73)90105-6
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1972EL12      Phys.Lett. 40B, 641 (1972)

C.Ellegaard, J.R.Lien, O.Nathan, G.Sletten, F.Ingebretsen, E.Osnes, P.O.Tjom, O.Hansen, R.Stock

The (1f₇/₂)² Multiplet in ⁴²Ca

NUCLEAR REACTIONS ⁴¹Ca(d, p), E=12 MeV; measured σ(Ep, θ). ⁴²Ca deduced levels, L(n), S.

doi: 10.1016/0370-2693(72)90617-X
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1972EL13      Phys.Lett. 41B, 97 (1972)

P.J.Ellis, E.Osnes

RPA Renormalisation of the Effective Interaction in a Hartree-Fock Basis

doi: 10.1016/0370-2693(72)90435-2
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1972EL14      Nucl.Phys. A196, 161 (1972)

P.J.Ellis, A.D.Jackson, E.Osnes

On the Number-Conserving Sets

doi: 10.1016/0375-9474(72)90958-X
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1972EL17      Phys.Lett. 42B, 335 (1972)

P.J.Ellis, E.Osnes

RPA Calculation of the Effective Charge in a Hartree-Fock Basis

doi: 10.1016/0370-2693(72)90501-1
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1971OS01      Phys.Lett. 34B, 113 (1971)

E.Osnes, T.T.S.Kuo, C.S.Warke

Core-Renormalization of the pf-Shell Effective Interaction for an RPA-Description of the Core

NUCLEAR STRUCTURE ⁴⁰Ca; calculated core polarization contribution to effective interaction. RPA.

doi: 10.1016/0370-2693(71)90682-4
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1971OS03      Nucl.Phys. A168, 190 (1971)

E.Osnes, T.T.S.Kuo, C.S.Warke

Core Polarization of the Effective Two-Nucleon Interaction for Different Descriptions of the Core

NUCLEAR STRUCTURE ¹⁶O; calculated levels. Core polarization effects.

doi: 10.1016/0375-9474(71)90658-0
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1970DA12      Nucl.Phys. A154, 12 (1970)

J.Damgaard, C.K.Scott, E.Osnes

Calculation of Coulomb Energy Differences

NUCLEAR STRUCTURE ¹⁶O, ²⁸Si, ³²S, ^40,48Ca, ²⁰⁸Pb; calculated monopole polarization, self-energy contributions to Coulomb energy differences.

doi: 10.1016/0375-9474(70)91065-1
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1970OS01      Nucl.Phys. A154, 331 (1970)

E.Osnes, C.S.Warke

Nuclear Structure Information from Isovector Electromagnetic Transitions in ⁵¹V

NUCLEAR STRUCTURE ⁵¹V; calculated levels, B(E2), μ.

doi: 10.1016/0375-9474(70)90161-2
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1969FE06      Nucl.Phys. A135, 545 (1969)

P.Federman, G.Greek, E.Osnes

Core-Particle Interaction and Fragmentation of Single-Particle Levels in ⁴¹Ca and ⁴¹Sc

NUCLEAR STRUCTURE ⁴¹Ca, ⁴¹Sc; calculated levels.

doi: 10.1016/0375-9474(69)90004-9
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1969OS01      Phys.Letters 30B, 306 (1969)

E.Osnes, C.S.Warke

On the Renormalization of the Effective Two-Nucleon Interaction by Core-Polarization Processes

NUCLEAR STRUCTURE ¹⁸O, ¹⁸F; calculated levels. Random phase approximation, core polarization corrections.

doi: 10.1016/0370-2693(69)90487-0
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1968OS01      Phys.Letters 26B, 274 (1968)

E.Osnes

Effective Three-Body Interactions in Ca-Isotopes

doi: 10.1016/0370-2693(68)90557-1
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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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