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Chinese Physics C> 1978, Vol. 2> Issue(3) : 263-266 

THE FINE STRUCTURE OF 208Pb 1+ STATES

  • The energy levels and transition probabilities B（M1） of the 208Pb 1+ states are calculated using the matrix diagonalized method in which the （1p 1h） configurations are coupled to collective octupole phonons. Calculated results show that the fine structure of the 208Pb giant magnectic resonance depends rather strongly on the phononparticle coupling constant.
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    [1] C. D. Bowman, Physical Review Letters, 25(1970), 1302.[2] L. W. Fagg et al., Review Modern Physics, 47(1975), 683.[3] S. Raman et al., "Proceedings of the International Conference on Nuclear Physics",Tokyo(1977), 454.[4] J. D. Vergados, Physics Letters, 36B(1971), 12.[5] P. Ring, J. Spech, Nuclear Physics, A235(1974), 315.[6] J. S. Dehesa et al., "Proceedings of the International Conference on Nuclear Physics ", Tokyo (1977), 452.

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FU TE-CHI and FANG PAO. THE FINE STRUCTURE OF 208Pb 1+ STATES[J]. Chinese Physics C, 1978, 2(3): 263-266.
FU TE-CHI and FANG PAO. THE FINE STRUCTURE OF 208Pb 1+ STATES[J]. Chinese Physics C, 1978, 2(3): 263-266. shu
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Received: 1977-12-30
Revised: 1900-01-01
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THE FINE STRUCTURE OF 208Pb 1+ STATES

  • Received Date: 1977-12-30
  • Accepted Date: 1900-01-01
  • Available Online: 1978-06-05

Abstract: The energy levels and transition probabilities B（M1） of the 208Pb 1+ states are calculated using the matrix diagonalized method in which the （1p 1h） configurations are coupled to collective octupole phonons. Calculated results show that the fine structure of the 208Pb giant magnectic resonance depends rather strongly on the phononparticle coupling constant.

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