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NSR database version of April 27, 2024.

Search: Author = P.Halse

Found 23 matches.

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1999EL04      J.Phys.(London) G25, 667 (1999)

J.P.Elliott, J.A.Evans, P.Halse

Mappings from Shell-Model SU(3) to Boson SU(3)

doi: 10.1088/0954-3899/25/4/016
Citations: PlumX Metrics


1999HA21      J.Phys.(London) G25, 867 (1999)

M.K.Harder, P.Halse, L.Frankland

Shell-Model Calculations Near N = Z = 28

NUCLEAR STRUCTURE 53,54,55Co, 52,53Fe, 55,58Ni, 60Zn; calculated levels, J, π. 55Ni, 55Co deduced high-K isomers. Shell model. Comparison with data.

doi: 10.1088/0954-3899/25/4/057
Citations: PlumX Metrics


1999HA22      J.Phys.(London) G25, 871 (1999)

P.Halse, M.K.Harder

An Investigation of Shell Model Structure Near 56Ni

NUCLEAR STRUCTURE 55Co, 56,57Ni; calculated level energies, B(E2), B(M1) parameter dependence. Shell model.

doi: 10.1088/0954-3899/25/4/058
Citations: PlumX Metrics


1996RO02      Phys.Rev. C53, R1465 (1996)

M.Robinson, P.Halse, W.Trinder, R.Anne, C.Borcea, M.Lewitowicz, S.Lukyanov, M.Mirea, Yu.Oganessian, N.A.Orr, Yu.Penionzhkevich, M.G.Saint-Laurent, O.Tarasov

New Isomer 32mAl

NUCLEAR REACTIONS 9Be(36S, X), E=75 MeV/nucleon; 9Be(40Ar, X), E=61 MeV/nucleon; measured (fragment)γ-coin, fragment mass distribution, γγ-coin; deduced evidence for 32mAl. 32Al deduced isomer T1/2, J, π, decay characteristics. Shell model comparison.

doi: 10.1103/PhysRevC.53.R1465
Citations: PlumX Metrics


1995HA47      Phys.Lett. 363B, 145 (1995)

P.Halse, P.Van Isacker, B.R.Barrett

Sum Rules of B(M1, 0+1 → 1+) Strength in IBM-3 and IBM-4

NUCLEAR STRUCTURE 20,22Ne, 24,26Mg; calculated summed B(M1). Isospin-invariant forms of the interacting boson model.

doi: 10.1016/0370-2693(95)01213-A
Citations: PlumX Metrics


1995KA14      Phys.Rev. C51, 2494 (1995)

S.Karataglidis, P.Halse, K.Amos

Transverse Electric Form Factors for Electron Scattering and Violation of Current Conservation in Nuclear Models

NUCLEAR REACTIONS 12C, 20Ne, 24Mg, 28Si(e, e), E not given; calculated transverse electric form factors. Projected Hartree-Fock transition densities, shell model.

doi: 10.1103/PhysRevC.51.2494
Citations: PlumX Metrics


1994JA08      Nucl.Phys. A571, 242 (1994)

L.Jaqua, P.Halse, B.R.Barrett, J.P.Vary

Effective Shell-Model Interaction for No-Core Model Spaces

NUCLEAR STRUCTURE 4He; calculated binding energy vs intermediate state excitation energy; deduced model convergence features. Effective shell-model interaction, no-core model spaces.

doi: 10.1016/0375-9474(94)90059-0
Citations: PlumX Metrics


1993HA04      Phys.Lett. 300B, 308 (1993)

P.Halse, S.J.Robinson

Shell Model-IBM Correspondence and the IBM Interpretation of 52Ti

NUCLEAR STRUCTURE 52Ti; calculated levels, B(λ), δ. Shell model, interacting boson model interpretation.

doi: 10.1016/0370-2693(93)91337-M
Citations: PlumX Metrics


1993HA37      J.Phys.(London) G19, 1859 (1993)

P.Halse

Shell-Model Calculations for the A ≈ 100 Region: Application to the even-Z N = 52 isotones 92Zr-100Cd

NUCLEAR STRUCTURE 90Y, 106,107Sn; calculated levels. 92Zr, 92Mo, 96Ru, 98Pd, 100Cd; calculated yrast spectra, E2, M1 matrix elements. 98Pd, 100Cd deduced shape features. Shell model.

doi: 10.1088/0954-3899/19/11/013
Citations: PlumX Metrics


1991HA08      Phys.Rev. C44, 562 (1991)

P.Halse

Reply to ' Comment on ' Comparison of Realistic and Symmetry-Determined S and D Pairs for 156Gd ' '

NUCLEAR STRUCTURE 156Gd; analyzed S-, D-pair determination criteria.

doi: 10.1103/PhysRevC.44.562
Citations: PlumX Metrics


1991HA26      Phys.Rev. C44, 2467 (1991)

P.Halse

Pair Condensates in Realistic Shell Model States. II. M1 States in 54,56Cr and 56,58,60Fe

NUCLEAR STRUCTURE 56,58,60Fe, 54,56Cr; calculated levels, B(λ). Shell model, pair condensates.

doi: 10.1103/PhysRevC.44.2467
Citations: PlumX Metrics


1990HA16      Phys.Rev. C41, 2340 (1990)

P.Halse

Pair Condensates in Realistic Shell Model States. I. 56Fe and 58Fe

NUCLEAR STRUCTURE 56,58Fe; calculated levels. Shell model states, SD pair condensates.

doi: 10.1103/PhysRevC.41.2340
Citations: PlumX Metrics


1989HA23      Ann.Phys.(New York) 192, 204 (1989)

P.Halse, B.R.Barrett

β-Decay and the Structure of Light Nuclei

NUCLEAR STRUCTURE A=20-36; calculated β-decay Gamow-Teller transition strengths; deduced T=0 state structure. Interacting boson model, SU(4) limit.

doi: 10.1016/0003-4916(89)90125-5
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1989SC11      Phys.Rev. C39, 2419 (1989)

H.A.Schmitt, P.Halse, A.B.Balantekin, B.R.Barrett

Noncompact Orthosymplectic Supersymmetry in 61Ni and 62Ni

NUCLEAR STRUCTURE 61,62Ni; calculated levels, B(λ); deduced supersymmetry classification scheme. Geometrical model, noncompact orthosymplectic supersymmetry.

doi: 10.1103/PhysRevC.39.2419
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1988BA47      Phys.Rev. C38, 1392 (1988)

A.B.Balantekin, B.R.Barrett, P.Halse

β Vibrations in the O(6) Limit of the Proton-Neutron Interacting Boson Model

NUCLEAR STRUCTURE 196Pt, 134Ba; calculated (β)-vibrational state energy. Proton-neutron interacting boson model, O(6) limit.

doi: 10.1103/PhysRevC.38.1392
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1987HA08      Phys.Rev. C35, 774 (1987); Erratum Phys.Rev. C35, 1964 (1987)

P.Halse, Z.Y.Pan

Comparison of SU(3) Phenomenologies in the sd Shell

NUCLEAR STRUCTURE 20,22Ne, 24,26,28Mg, 20F, 22,24Na, 26,28Al; calculated band structure, characteristic parameters. Dynamical symmetries, shell model.

doi: 10.1103/PhysRevC.35.774
Citations: PlumX Metrics


1987HA16      Phys.Rev. C36, 372 (1987)

P.Halse

Test of the Fermion Dynamical Symmetry Model Microscopy in the sd Shell

NUCLEAR STRUCTURE 20,22Ne, 24Mg; calculated realistic wave function overlap square. Fermion dynamical symmetry model.

doi: 10.1103/PhysRevC.36.372
Citations: PlumX Metrics


1987HA41      Phys.Rev. C36, 2611 (1987)

P.Halse, J.N.Ginocchio

SU(3) X SU(4) Limit of an Isospin Invariant Fermion Dynamical Symmetry Model

NUCLEAR STRUCTURE 20,22Ne, 24Mg, 16O; calculated levels, band structure; deduced symmetry classification.

doi: 10.1103/PhysRevC.36.2611
Citations: PlumX Metrics


1985BA25      Phys.Lett. 155B, 133 (1985)

B.R.Barrett, P.Halse

M1 Transition Strength in the SU(3) Limit of the Generalized IBM-2

NUCLEAR STRUCTURE 156Gd; analyzed B(M1) interpretation. Interacting boson model, generalized SU(3) limit, arbitrarily large boson number.

doi: 10.1016/0370-2693(85)90972-4
Citations: PlumX Metrics


1985HA15      Phys.Lett. 156B, 1 (1985)

P.Halse

On a Microscopic Interpretation of the IBM in the sd Shell

NUCLEAR STRUCTURE 20Ne, 20O; calculated sd shell model analogs of IBM-4 states.

doi: 10.1016/0370-2693(85)91343-7
Citations: PlumX Metrics


1985HA27      Nucl.Phys. A445, 93 (1985)

P.Halse

An Application of the Interacting Boson Model to the First Half of the s-d Shell (II). Odd-odd nuclei

NUCLEAR STRUCTURE 22Na, 26Al; calculated levels, magnetic dipole, electric quadrupole operator reduced matrix elements. Interacting boson model.

doi: 10.1016/0375-9474(85)90362-8
Citations: PlumX Metrics


1985HA29      Phys.Lett. 162B, 15 (1985)

P.Halse

An SU(3) Analysis of 22Ne

NUCLEAR STRUCTURE 22Ne; calculated levels, band structure, symmetry characteristics.

doi: 10.1016/0370-2693(85)91051-2
Citations: PlumX Metrics


1984HA14      Nucl.Phys. A417, 301 (1984)

P.Halse, J.P.Elliott, J.A.Evans

An Application of the Interacting Boson Model to the First Half of the sd Shell (1). Even-Even Nuclei

NUCLEAR STRUCTURE 20,22,24Ne, 20,22O, 20,24,26,28Mg, 28Si; calculated levels, B(E2), binding energies relative to 16O. Interacting boson model.

doi: 10.1016/0375-9474(84)90510-4
Citations: PlumX Metrics


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