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Extra resources for Band Structure and Nuclear Dynamics. Proceedings of the International Conference on Band Structure and Nuclear Dynamics Tulane University, New Orleans

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We assume that the low-lying states from the basis states of two bosons, S*"" α. , a. 2 =3-. 30). 31) become can be constructed 1argely = S.. ' and T"** = S 2 . *α. *3. = Σ 3 *a. 33) . 27) conserves the total number of bosons, this translates into the conservation of . 32) unless we can assume that N m « N and we shall therefore proceed with this assumption. 36) Retaining only the first two terms under the radical and expanding the remainder to first order only - to illustrate procedure - we derive an approximate boson Hamiltonian of the form H B = Hd + H od ' (4 '37) where H, is diagonal in the direct product basis constructed from St* and T*t* and is given by the expression 26 A.

Phys. A309 (1978)1. T. Otsuka, Unpublished thesis, Dept. of Physics, U. of Tokyo (1978). S. C. Pang, A. Klein, and R. M. Dreizler, Ann. of Phys. ) £9 (1968) 477. M. Kleber, Phys. Letters 30B (1969) 588. M. Vallieres, A. Klein, and R, M. Dreizler, Phys. Rev. Cl_ (1973) 2188. T. Marumori, M. Yamamura, and A. Tokunaga, Prog. Theoret. Phys. (Kyoto) 31_ (1964) 1009. S. Y. Li, R. M. Dreizler and A. Klein, Phys. Rev. C£ (1971) 1571. 50. 51. 52. 53. 54. 55. T. Holstein and H. Primakoff, Phys. Rev. 58^ (1950) 1098.

32) unless we can assume that N m « N and we shall therefore proceed with this assumption. 36) Retaining only the first two terms under the radical and expanding the remainder to first order only - to illustrate procedure - we derive an approximate boson Hamiltonian of the form H B = Hd + H od ' (4 '37) where H, is diagonal in the direct product basis constructed from St* and T*t* and is given by the expression 26 A. KLEIN H-, = e , S t S a 1 + V + 12,12 e0TfT 2 S+T+TS + V 22,22 T+T+TT (4 / '38) where, with the definitionX r.

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