REARRANGEMENT EFFECTS IN SHELL-MODEL CALCULATIONS USING DENSITY-DEPENDENT INTERACTIONS

[1]  H. Nann,et al.  HIGH-SPIN 1P-1H CONFIGURATIONS IN SN-116 AND THEIR FRAGMENTATION AS SEEN IN THE REACTIONS SN-116(-]P,P'), SN-116(E,E'), IN-115(3HE,D) AND IN-115(ALPHA, T) , 1986 .

[2]  G. T. Velde,et al.  Spectroscopy of even Sn nuclei and generalized-seniority breaking , 1985 .

[3]  M. Brack,et al.  Static nuclear properties and the parametrisation of Skyrme forces , 1984 .

[4]  M. Waroquier,et al.  An effective Skyrme-type interaction for nuclear structure calculations , 1983 .

[5]  S. M. Wong,et al.  Topics in Nuclear Physics I , 1981 .

[6]  A. Klein.  Nuclear collective motion. , 1980, Science.

[7]  M. Waroquier,et al.  The extended Skyrme force versus realistic interactions: Application on 42Ca , 1979 .

[8]  S. Adachi,et al.  Particle-hole type matrix elements for density-dependent interactions , 1979 .

[9]  P. Ellis,et al.  An introductory guide to effective operators in nuclei , 1977 .

[10]  D. Gogny,et al.  Theory of elementary excitations in closed shell nuclei , 1977 .

[11]  A. Faessler,et al.  On the use of Skyrme forces in self-consistent RPA calculations , 1977 .

[12]  K. Liu,et al.  A self-consistent microscopic description of the giant resonances including the particle continuum , 1976 .

[13]  K. Liu,et al.  Giant multipole resonances , 1976 .

[14]  H. Köhler.  Skyrme force and the mass formula , 1976 .

[15]  P. Quentin,et al.  Nuclear ground-state properties and self-consistent calculations with the skyrme interaction: (I). Spherical description , 1975 .

[16]  M. Waroquier,et al.  A phase-consistent derivation of the electromagnetic multipole operators , 1975 .

[17]  P. Ring,et al.  Nuclear structure calculations with a density-dependent force in 208Pb , 1974 .

[18]  J. Speth,et al.  Calculation of higher multipole resonances , 1974 .

[19]  W. F. Gunsteren,et al.  The FBCS model and the inverse gap equations applied to the tin isotopes , 1974 .

[20]  T. Kuo.  Shell-Model Effective Interactions and the Free Nucleon-Nucleon Interaction , 1974 .

[21]  D. Sprung,et al.  Spherical nuclei in the local density approximation , 1972 .

[22]  E. Boeker,et al.  Comparison between the bcs and the FBCS formalisms as approximations to the low-seniority shell model , 1971 .

[23]  G. E. Brown,et al.  Reaction matrix elements for the 0f-1p shell nuclei , 1968 .

[24]  A. Migdal.  Theory of Finite Fermi Systems and Application to Atomic Nuclei , 1967 .

[25]  G. E. Brown,et al.  Structure of finite nuclei and the free nucleon-nucleon interaction: General discussion of the effective force , 1967 .

[26]  T. Kuo.  Structure of finite nuclei and the free nucleon-nucleon interactions: (II). Core polarization and effective interactions for the nickel isotopes , 1967 .

[27]  G. E. Brown,et al.  Structure of finite nuclei and the free nucleon-nucleon interaction: An application to 18O and 18F , 1966 .

[28]  N. Mau,et al.  Particle-hole description of carbon 12 and oxygen 16 , 1964 .

[29]  V. Gillet.  The phenomenology of the effective two-body forces for C12 and O16 in the particle-hole models , 1964 .

[30]  A. Messiah,et al.  The canonical form of an antisymmetric tensor and its application to the theory of superconductivity , 1962 .

[31]  M. Baranger.  Extension of the Shell Model for Heavy Spherical Nuclei , 1960 .

[32]  D. Thouless.  Stability conditions and nuclear rotations in the Hartree-Fock theory , 1960 .

[33]  N. Bogolyubov.  Reviews of Topical Problems: the Compensation Principle and the Self-Consistent Field Method , 1959 .

[34]  C. Bloch,et al.  Sur la détermination des premiers états d'un système de fermions dans le cas dégénéré , 1958 .

[35]  K. Ford,et al.  SHELL-MODEL THEORY OF Pb$sup 20$$sup 6$ , 1958 .

[36]  J. Valatin.  Comments on the theory of superconductivity , 1958 .