An IBM-3 analysis of the nuclei just beyond the magic numbers N = Z = 28

[1]  J. Elliott,et al.  Electromagnetic operators in IBM-3 and their dependence on the boson number and isospin , 1996 .

[2]  G. Long,et al.  An IBM-3 hamiltonian from a multi-j-shell model , 1995 .

[3]  G. Long,et al.  A comparison of the IBM-1 projections from IBM-2 and IBM-3 , 1995 .

[4]  A. H. Wapstra,et al.  The 1993 atomic mass evaluation: (I) Atomic mass table , 1993 .

[5]  G. Long,et al.  A microscopic derivation of the dependence of the IBM3 hamiltonian on the boson number and isospin , 1993 .

[6]  M. Thompson,et al.  On the role of isoscalar bosons in lighter nuclei , 1989 .

[7]  P. Raghavan,et al.  Table of nuclear moments , 1989 .

[8]  J. Elliott,et al.  Isospin in a boson approximation for particles and holes , 1987 .

[9]  J. P. Elliott The interacting boson model of nuclear structure , 1985 .

[10]  J. Elliott,et al.  An application of the interacting boson model to the first half of the sd shell: (I). Even-even nuclei , 1984 .

[11]  T. Otsuka Rotational states and interacting bosons , 1981 .

[12]  J. Evans,et al.  An intrinsic spin for interacting bosons , 1981 .

[13]  J. P. Elliot,et al.  An isospin invariant form of the interacting boson model , 1980 .

[14]  H. Stroke,et al.  Theory of the Nuclear Shell Model , 1980 .

[15]  Francesco Iachello,et al.  Interacting boson model of collective nuclear states IV. The O(6) limit , 1979 .

[16]  T. Otsuka,et al.  Nuclear Shell Model and Interacting Bosons , 1978 .

[17]  A. Arima,et al.  COLLECTIVE NUCLEAR STATES AS SYMMETRIC COUPLINGS OF PROTON AND NEUTRON EXCITATIONS , 1977 .

[18]  K. T. Hecht,et al.  GENERALIZED SENIORITY FOR FAVORED J # 0 PAIRS IN MIXED CONFIGURATIONS , 1969 .

[19]  K. Hecht Five-dimensional quasi-spin the n , T dependence of shell-model matrix elements in the seniority scheme , 1967 .