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NSR database version of April 27, 2024.

Search: Author = A.Holt

Found 11 matches.

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2002FO03      Phys.Rev. C65, 044303 (2002)

N.Fotiades, J.A.Cizewski, J.A.Becker, L.A.Bernstein, D.P.McNabb, W.Younes, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, A.Holt, M.Hjorth-Jensen

High-Spin Excitations in ^{92, 93, 94, 95}Zr

NUCLEAR REACTIONS ¹⁷³Yb(²⁴Mg, X), E=134.5 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission. ^92,93,94,95Zr deduced high-spin levels, J, π, configurations. Gammasphere array.

doi: 10.1103/PhysRevC.65.044303
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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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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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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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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
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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 ^{102,104,106,108,110,112,105,107}Sn; 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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