Deep proton-hole states in 147Pr, 151Pm and 155Eu

[1]  S. Gales,et al.  Damping of high-lying single-particle modes in heavy nuclei , 1988 .

[2]  C. Blyth,et al.  Elastic scattering of 33 MeV tritons and isospin dependence of mass-3 optical potential , 1987 .

[3]  D. Miller,et al.  Deeply-bound hole states in 57Co and the spreading of the 1d52 hole strength distribution , 1987 .

[4]  Witold Nazarewicz,et al.  Single-particle energies, wave functions, quadrupole moments and g-factors in an axially deformed woods-saxon potential with applications to the two-centre-type nuclear problems , 1987 .

[5]  N. Blasi,et al.  Proton hole response function on 196Pt and 197Au transitional target nuclei up to high excitation energy , 1987 .

[6]  W. T. Milner,et al.  Transition probability, B(E2)up-arrow, from the ground to the first-excited 2/sup +/ state of even-even nuclides , 1987 .

[7]  K. Knöpfle,et al.  Study of the (d, 3He) reaction on 84Kr and 86Kr and the lowest moments of the proton strength distributions in the Zr region , 1986 .

[8]  D. G. Burke,et al.  Two-quasiproton states in 168Er studied by the 169Tm(t, α)168Er reaction , 1985 .

[9]  J. Wiele,et al.  High-lying valence and inner-proton-hole states in 207Tl via the (d, 3He) reaction at 108 MeV , 1984 .

[10]  C. Stoyanov,et al.  High-lying single-proton states in spherical nuclei , 1983 .

[11]  C. Stoyanov,et al.  Nuclear properties in the lead region within the quasiparticle-phonon nuclear model , 1983 .

[12]  S. Gales,et al.  Neutron-hole strength distributions in heavy nuclei: (II). The 144, 148, 152Sm(3He, α) 143, 147, 151Sm and the 144, 148, 150, 152, 154Sm(p, d) 143, 147, 149, 151, 153Sm reactions , 1983 .

[13]  R. Broglia,et al.  Damping of nuclear excitations , 1983 .

[14]  R. Broglia,et al.  Role of the nuclear surface in a unified description of the damping of single-particle states and giant resonances , 1981 .

[15]  S. Gales High-lying neutron hole strengths observed in pick-up reactions , 1981 .

[16]  K. Knöpfle,et al.  Spin determination of deeply-bound hole states from ( $$\vec d$$ ,3He) reactions , 1980 .

[17]  C. Stoyanov,et al.  The description of the fragmentation of one-quasiparticle states in spherical nuclei , 1980 .

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

[19]  C. Stoyanov Iterative method of solving the equations of the quasiparticle-phonon model in spherical nuclei , 1979 .

[20]  K. Knöpfle,et al.  Strong exhaustion of 1gsol92 strength by deeply-bound proton-hole states in Pm isotopes , 1979 .

[21]  D. G. Burke,et al.  Single-proton states in 155Eu , 1979 .

[22]  W. B. Ewbank,et al.  Nuclear data sheets for A = 147 , 1978 .

[23]  F. Perey,et al.  Compilation of phenomenological optical-model parameters 1954–1975 , 1976 .

[24]  V. Solovʹev Theory of complex nuclei , 1976 .

[25]  D. G. Burke,et al.  A nuclear structure study of 165Ho using the (t, α), (α, t) and (3He, d) reactions , 1975 .

[26]  B. S. Nielsen,et al.  Equilibrium deformations and excitation energies for non-collective states in odd-Z rare-earth nuclei , 1975 .

[27]  V. G. Solov’ev,et al.  Model for describing the fragmentation of one- and many-particle states over the levels of an odd spherical nucleus , 1974 .

[28]  B. Sinha,et al.  Level structure of $sup 147$Pm , 1974 .

[29]  J. C. Waddington,et al.  The level structure of 151Pm , 1972 .

[30]  B. Elbek,et al.  Single Nucleon Transfer in Deformed Nuclei , 1969 .