E0 transitions in the γ-unstable nucleus 124Te
暂无分享,去创建一个
K. Schreckenbach | G. Colvin | K. Kumar | W. Hamilton | A. Subber | P. Park
[1] J. Elliott,et al. A soluble γ-unstable hamiltonian , 1986 .
[2] R. Bünde. Contributions to INTOR , 1986 .
[3] J. Elliott,et al. A study of the γ-unstable nucleus 124Te , 1985 .
[4] R. Casten,et al. An extensive region of O(6)-like nuclei near A = 130 , 1985 .
[5] A. Irbäck,et al. Mixed-Symmetry interacting-Boson-Model states in the nuclei Ba140, Ce142, and Nd144 with N=84 , 1984 .
[6] O. Scholten,et al. ON MAGNETIC DIPOLE PROPERTIES IN THE NEUTRON PROTON IBA MODEL , 1984 .
[7] N. M. Stewart,et al. Low energy nuclear states in124Te , 1984 .
[8] S. Ohya,et al. Nuclear data sheets for A = 124 , 1984 .
[9] S. J. Robinson,et al. Levels and transitions in 124Te following thermal-neutron capture by 123Te and the beta decay of oriented 124Sb , 1983 .
[10] K. Schreckenbach,et al. Strengths of E0 transitions in 188Os and 196Pt and the structure of IBA wavefunctions in the OsPt transition region , 1982 .
[11] M. Sambataro. A study of Cd and Te isotopes in the interacting boson approximation , 1982 .
[12] J. Hamilton,et al. E0-E2-M1 multipole admixtures of transitions in even-even nuclei , 1982 .
[13] R. Peterson,et al. The reaction 14C(3He, n)16O and the coexistence model of 16O , 1981 .
[14] B. Barrett,et al. Interacting boson approximation model of the tungsten isotopes , 1981 .
[15] O. Scholten,et al. COLLECTIVE QUADRUPOLE STATES OF XE, BA AND CE IN THE INTERACTING BOSON MODEL , 1980 .
[16] P. A. Baker,et al. Σ+ and Y*+ (1385) production in line-reversed π+p and K-p reactions at 7 GeV/c , 1980 .
[17] Francesco Iachello,et al. Interacting boson model of collective nuclear states IV. The O(6) limit , 1979 .
[18] A. K. Sharma,et al. Level Structure of124Te , 1979 .
[19] K. Schreckenbach,et al. The double focusing iron-core electron-spectrometer “BILL” for high resolution (n, e−) measurements at the high flux reactor in Grenoble , 1978 .
[20] P. Aguer,et al. Deformed-quasiparticle basis for calculating potential energy surfaces and nuclear spectra , 1977 .
[21] I. Hall,et al. Quadrupole moments of the first 2+ states of doubly even nuclei in the Z=50 region , 1977 .
[22] F. Boehm,et al. Changes of mean-square nuclear charge radii from isotope shifts of electronic Kα X-rays , 1974 .
[23] K. Kumar. Collective Hamiltonian derived from the pairing-plus-quadrupole model , 1974 .
[24] R. Haroutunian,et al. Investigation of the reorientation effect onTe122,Te124,Te126,Te128, andTe130 , 1974 .
[25] W. Myers,et al. The nuclear droplet model for arbitrary shapes , 1974 .
[26] K. C. Mann,et al. The Decay of 124Sb , 1974 .
[27] F. Bertrand. Nuclear data sheets for A = 124 , 1973 .
[28] J. D. King,et al. The electromagnetic interaction , 1973 .
[29] J. B. Ball,et al. Energy levels of 122,124Te populated by (3He, d) AND (p, t) reactions , 1972 .
[30] V. Trusov. Internal conversion coefficients for high-energy transitions , 1972 .
[31] W. Greiner,et al. Collective potential energy surfaces and nuclear structure , 1971 .
[32] D. A. Bell,et al. Table of EO conversion probability electronic factors , 1970 .
[33] A. Bäcklin,et al. Decay properties of the 99 and 130 keV levels in 195Pt , 1970 .
[34] W. Walters,et al. Levels of Te-124 from the Decay of 4.2-Day I-124 , 1969 .
[35] M. Baranger,et al. Nuclear deformations in the pairing-plus-quadrupole model: (V). Energy levels and electromagnetic moments of the W, Os and Pt nuclei , 1968 .
[36] M. Baranger,et al. NUCLEAR DEFORMATIONS IN THE PAIRING-PLUS-QUADRUPOLE MODEL. II. JUSTIFICATION OF THE MODEL. , 1967 .
[37] M. Baranger,et al. COMPLETE NUMERICAL SOLUTION OF BOHR'S COLLECTIVE HAMILTONIAN. , 1967 .
[38] J. Rasmussen. Theory of E0 transitions of spheroidal nuclei , 1960 .
[39] E. Church,et al. Electric-Monopole Transitions in Atomic Nuclei , 1955 .