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By A. L. Goodman

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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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S . 02 — n ■ Sm I50L k - _ / 0 1 1 1 50 1 L__l Q2 1 1 1 1 1 100 I Opfern4] 1 1 J 150 1 1 1 200 Fig. 14. Linear plot of *ί02 v s · Qo2· Predictions from the two-fluid model are shown by crosses, empirical values by open circles. 6) x lO""24 cm 2 (keV) 1 / 2 . The Q 0 2 values for the heaviest actinide nuclei increase by almost 50%, while the «/Q2 values remain approximately constant. PRESENT STATUS OF THE VMI AND RELATED MODELS 49 ACKNOWLEDGEMENTS It is a pleasure to express my warm gratitude to the many associates who were essential in helping, step by step, to reveal secrets so closely guarded by Nature.

82 only bands for singly and doubly magic nuclei occur (with one exception, which will be discussed in section 2). The interpretation of this behavior is quite obvious: The higher the "threshold energy" γ 40 2, the more does the nucleus resist cranking. e. 82, the nucleus, now being perfectly spherical, can only be excited by promoting one or two nucleon pairs to a higher orbit, thus bringing about deformation, which permits cranking from the 2+ state on. Das, Dreizler and Klein9) presented a proof showing that the VMI and Harris models are equivalent to all orders.

Phys. A302 (1978) 214). I am indebted to L. Zamick for this suggestion. A. S. Goldhaber and G. Scharff-Goldhaber, Phys. Rev. C 17 (1978) 1171. J. D. Garrett, G. Scharff-Goldhaber and J. P. Vary, Bull. Am. Phys. Soc. 19 (1974) 59. B. Buck, L. C. Biedenharn and R. Y. Cusson, Nucl. Phys. A317 (1979) 205. J. N. Ginocchio and M. W. Kirson, Proc. Int. Conf. on band structure and nuclear dynamics, New Orleans, 1980, ed. A. L. Goodman, Vol. 1, contributed papers, p. 38. W. Andrejtscheff, E. Nadjakov and Ts.

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