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NSR database version of May 3, 2024.

Search: Author = M.W.Kirson

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2013ZA08      Phys.Rev. C 87, 067302 (2013)

L.Zamick, A.Escuderos, S.J.Q.Robinson, Y.Y.Sharon, M.W.Kirson

Isobaric analog states in the f_7/2 and g_9/2 shells

NUCLEAR STRUCTURE ^44,46Sc, ^44,46Ca, ⁵²Mn, ⁵²Cr, ⁶⁰Cu, ⁶⁰Ni, ⁹⁴Rh, ⁹⁴Ru, ⁹⁶Ag, ⁹⁶Pd; calculated Coulomb energy estimates for pairs of nuclei using various mass formulas. ^44,46Sc, ⁵²Mn, ⁶⁰Cu, ⁹⁴Rh, ⁹⁶Ag; calculated energies of isobaric analog states (IAS) with T=2 and 3 using binding energy formulas and Coulomb energies, and shell-model. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.067302
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2012KI19      Nucl.Phys. A893, 27 (2012)

M.W.Kirson

An empirical study of the Duflo-Zuker mass formula

COMPILATION Z=42-54, 100-126; calculated, evaluated mass excess using Duflo-Zuker mass formula; deduced formula parameters.

doi: 10.1016/j.nuclphysa.2012.09.001
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2009GE09      Phys.Rev. C 80, 024307 (2009)

A.Gelberg, H.Sakurai, M.W.Kirson, S.Heinze

Wigner energy and shell gaps in two-nucleon separation energies

NUCLEAR STRUCTURE Z=10-26 (even), N=10-26(even); calculated two-proton and two-neutron separation energies for N=Z nuclei from binding energy formula. Discussed implications for Wigner energy and shell-gaps. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.024307
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2008KI01      Nucl.Phys. A798, 29 (2008)

M.W.Kirson

Mutual influence of terms in a semi-empirical mass formula

ATOMIC MASSES A=1-260; analyzed mass; deduced effect of additional terms in semi-empirical mass formula.

doi: 10.1016/j.nuclphysa.2007.10.011
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2007KI01      Nucl.Phys. A781, 350 (2007)

M.W.Kirson

Oscillator parameters in nuclei

NUCLEAR STRUCTURE A=1-250; analyzed radii; deduced oscillator strength parameters.

doi: 10.1016/j.nuclphysa.2006.10.077
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2007KI20      Phys.Rev. C 76, 064305 (2007)

M.W.Kirson, J.A.Mizrahi

Random interactions with isospin

doi: 10.1103/PhysRevC.76.064305
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2000KI31      Phys.Rev. C62, 057306 (2000)

M.W.Kirson

Equivalence of Interacting Boson Approximation-2 Hamiltonians in the Subspace of Maximum F Spin

doi: 10.1103/PhysRevC.62.057306
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1990LE21      Phys.Rev.Lett. 65, 2853 (1990)

A.Leviatan, J.N.Ginocchio, M.W.Kirson

Proton-Neutron Deformations and F-Spin Symmetry in Nuclei

NUCLEAR STRUCTURE ¹⁶⁵Ho; calculated ground state band F-spin mixing; deduced proton, neutron deformations role.

doi: 10.1103/PhysRevLett.65.2853
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1985KI14      Phys.Rev.Lett. 55, 2846 (1985); Erratum Phys.Rev.Lett. 56, 788 (1986)

M.W.Kirson, A.Leviatan

Resolution of Any Interacting-Model Hamiltonian into Intrinsic and Collective Parts

NUCLEAR STRUCTURE ¹⁴⁸Sm, ¹⁶⁸Er; calculated levels. Interacting boson model.

doi: 10.1103/PhysRevLett.55.2846
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1982KI03      Phys.Lett. 108B, 237 (1982)

M.W.Kirson

Isoscalar E3 Strength Distributions in Even-Even Nuclei

NUCLEAR STRUCTURE A=5-240; analyzed octupole strength systematics. Schematic model.

doi: 10.1016/0370-2693(82)91183-2
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1980GI08      Nucl.Phys. A350, 31 (1980)

J.N.Ginocchio, M.W.Kirson

An Intrinsic State for the Interacting Boson Model and Its Relationship to the Bohr-Mottelson Model

NUCLEAR STRUCTURE ^{148,150,152,154}Sm, ^{186,188,190,192,194,196}Pt, ^{112,124,134,136}Ce; calculated energy surfaces vs shape variables, intrinsic state orientation; deduced relation to Bohr-Mottelson model. Interacting boson approximation.

doi: 10.1016/0375-9474(80)90387-5
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1980KI02      Nucl.Phys. A337, 194 (1980)

M.W.Kirson

Electric Quadrupole Strength in Nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca; calculated B(E2), energy-weighted sum rule. Schematic model, coupling high-, low-lying quadrupole modes.

doi: 10.1016/0375-9474(80)90051-2
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1978KI04      Nucl.Phys. A301, 93 (1978)

M.W.Kirson

Model Dependence of Energy-Weighted Sum Rules

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ⁴⁰Ca; calculated potential parameters.

doi: 10.1016/0375-9474(78)90131-8
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1976HO14      Nucl.Phys. A266, 138 (1976)

H.M.Hofmann, Y.Starkand, M.W.Kirson

Perturbation Theory and Pade Approximants in Realistic Large-Matrix Models of the Nuclear Effective Interaction

NUCLEAR STRUCTURE ¹⁸O; calculated energy matrices for J, π, T=0, +, 1 states.

doi: 10.1016/0375-9474(76)90287-6
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1976KI01      Nucl.Phys. A257, 58 (1976)

M.W.Kirson

Giant Isoscalar Monopole States in Light Doubly Even Nuclei

NUCLEAR STRUCTURE ⁴He, ¹²C, ¹⁶O, ²⁸Si, ³²S, ⁴⁰Ca; calculated centroids of unobserved E0 strength.

doi: 10.1016/0375-9474(76)90475-9
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1975ST03      Phys.Lett. 55B, 125 (1975)

Y.Starkand, M.W.Kirson

Single-Particle Energies, Large-Matrix Diagonalizations and Perturbation Theory of Nuclear Effective Interactions

NUCLEAR STRUCTURE ¹⁸O; calculated levels, two-body effective interaction matrix elements.

doi: 10.1016/0370-2693(75)90422-0
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1973KI08      Phys.Lett. 47B, 110 (1973)

M.W.Kirson

Spin-Tensor Decomposition of Nuclear Effective Interactions

NUCLEAR STRUCTURE ¹⁶O, ⁴⁸Ca, ⁴⁸Sc; calculated levels.

doi: 10.1016/0370-2693(73)90582-0
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1972RA06      Phys.Lett. 38B, 162 (1972)

J.Rajewski, M.W.Kirson

Force Dependence of 0⁺ States in ²⁰⁸Bi

NUCLEAR STRUCTURE ²⁰⁸Bi; calculated levels, wave functions. Reaction matrix from Sussex, Tabakin potentials.

doi: 10.1016/0370-2693(72)90039-1
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1972RA08      Nucl.Phys. A181, 409 (1972)

J.Rajewski, M.W.Kirson

4p-2h Intermediate States and the Effective Interaction in Mass-18 Nuclei

NUCLEAR STRUCTURE A=18; analyzed 4p-2h intermediate states, effective interaction.

doi: 10.1016/0375-9474(72)90492-7
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1969ST15      Nucl.Phys. A137, 289 (1969)

M.M.Stingl, M.W.Kirson

Separable Structure of a Self-Consistent Potential in the Reaction-Matrix Theory of Nuclei

NUCLEAR STRUCTURE ¹⁶O; calculated wave functions for unbound states. Reaction matrix theory, self-consistent potential.

doi: 10.1016/0375-9474(69)90111-0
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