On the collective modes of infinite nuclear matter

[1]  A. D. Jackson,et al.  Collective states in nuclei a tale of two sounds , 1980 .

[2]  M. Greenfield,et al.  Search for isobaric analogues of M1 states and giant spinflip resonances in the 208Pb(p, n) reaction , 1980 .

[3]  M. Greenfield,et al.  Gamow-Teller matrix elements from 0/sup 0/ ( p,n) cross section , 1980 .

[4]  M. Greenfield,et al.  Observation of Giant Particle-Hole Resonances in 90-Zr(p,n)90-Nb , 1980 .

[5]  W. Alberico,et al.  Perturbative calculation of the compression modulus in the problem of the degenerate electron liquid , 1980 .

[6]  S. Stringari,et al.  Time-dependent Hartree-Fock polarizability and random phase approximation sum rules: (I). Theory , 1978 .

[7]  S. Stringari,et al.  Time-dependent Hartree-Fock polarizability and random phase approximation sum rules: (II). Application to isovector monopole, quadrupole and dipole excitations , 1978 .

[8]  D. Gogny,et al.  The propagation and damping of the collective modes in nuclear matter , 1977 .

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

[10]  G. Bertsch,et al.  On the macroscopic theory of the giant dipole state , 1976 .

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

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

[13]  D. Brink,et al.  Hartree-Fock Calculations with Skyrme's Interaction. I. Spherical Nuclei , 1972 .

[14]  G. E. Brown.  Landau, Brueckner-Bethe, and Migdal Theories of Fermi Systems , 1971 .

[15]  G. Bertsch,et al.  Effective mass in nuclei , 1968 .

[16]  S. P. Pandya.  NUCLEON-HOLE INTERACTION IN jj COUPLING , 1956 .