New positive-parity states and the shell-model description of 111Sn

[1]  W. Enghardt,et al.  In-beam study and structure of the N = 82 nucleus 141Pr , 1981 .

[2]  U. Hagemann,et al.  Structure of high-spin states in 143Pm , 1980 .

[3]  H. Blok,et al.  High-resolution investigation of the 112Sn(p, d)111Sn reaction , 1980 .

[4]  U. Hagemann,et al.  Collective excitations in the 117, 119, 121Te nuclei , 1979 .

[5]  M. Waroquier,et al.  Collective bands in even mass Sn isotopes , 1979 .

[6]  N. Yoshikawa,et al.  Study of high-spin states in odd sn isotopes , 1979 .

[7]  W. F. Gunsteren,et al.  Number-projected three-quasiparticle description of the odd Sn isotopes , 1978 .

[8]  W. F. Gunsteren,et al.  Influence of an enlargement of the model space on number projected quasiparticle calculations , 1976 .

[9]  L. Westerberg,et al.  Excited States in Odd Sn Nuclei, A = 109-125 , 1976 .

[10]  L. Westerberg,et al.  An in-beam electron-gamma spectrometer , 1975 .

[11]  T. Shibata,et al.  Low-lying states in 95Tc studied with the 93Nb(α, 2nγ)95Tc reaction , 1975 .

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

[13]  M. Singh,et al.  Decay of the light antimony isotopes 110, 111, 112, 114sb following the 112, 114Sn (p, xn) reactions , 1972 .

[14]  D. Clark,et al.  Nuclear isomers in 113Sn, 111Sn, 117Te and 115Te , 1972 .

[15]  J. Turner,et al.  A STUDY OF THE NUCLEAR STRUCTURE OF THE ODD TIN ISOTOPES BY MEANS OF THE (p,d) REACTION. , 1970 .

[16]  B. Wildenthal.  Shell model for N=82 nuclei , 1969 .

[17]  E. Seltzer,et al.  INTERNAL CONVERSION TABLES. PART I. K,L,M-SHELL CONVERSION COEFFICIENTS. , 1968 .

[18]  T. Yamazaki.  Tables of coefficients for angular distribution of gamma rays from aligned nuclei , 1967 .