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The energy for this path as a function of e is illustrated in Fig. II-7. 5, at larger e the energy starts to rise again quite rapidly. This is believed to arise primarily from the failure of the constraint of constant volume within any equipotential surface to conserve constant density. 7 £ Fig. II-7. Single particle model calculation of energy as a function of the deformation parameter e after minimization of the energy with respect to variation of e4. The rise in energy at large deformations illustrates the failure of the single particle model when the surface to volume ratio has increased greatly.
The Fission Barrier (Л c JD o o o Double r Vibrations 4-f"6+ 2+ -5 + —o+ K=0 c o *o Q_ X UJ o » o a> ■S E c P >^ 4+ 3+ 2+ K=2 Y/ o ^4 CD 1 £ E T3 c c ■o >4 o < GO a> B c a> GO o 5 (Л 53- c D O 1- O 6+ 4+ 2 + K=0 K=l Yi Y| E <л o < "oi K=2 K=3 4+ 3+ 2+ 1+ K=l 3 - Уз 0 +Уз; 21- Y^ Y3° 0+ K=C Fig. If-17. Schematic diagram of some possible collective band structures for an eveneven transition nucleus with a stable quadrupole deformation. The ^-vibration band (Y2) is missing because it is a vibration in the fission direction.
Lin, W. (1970). Phys. Rev. C 2, 871. , and Nilsson, S. G. (1970). Phys. Lett. B 31, 283. , Nilsson, S. , and Wycech, S. (1969). Phys. Lett. B 30, 223. Mosel, U. (1972). Phys. Rev. C 6, 971. Mottelson, B. , and Nilsson, S. G. (1959). Kgl. Dan. Vidensk. Selsk. Mat. Fys. Skr. 1, No. 8. Muzychka, Yu. , Pashkevich, V. , and Strutinsky, V. M. (1969). Sov. J. Nucl. Phys. 8, 417. Myers, W. , and Swiatecki, W. J. (1966). Nucl. Phys. 81, 1. Myers, W. , and Swiatecki, W. J. (1967). Proc. Int. Symp. "Why and How Should We Investigate Nuclides Far off the Stability Line," Lysekil, Sweden, August 21-27, 1966, p.