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36) The quadrupole and octupole states are considered in the calculations only. The position of the lowest state for the all nuclei, with exception of 208Pb, was defined by phenomenological equations which reproduced the experimental data well enough for middle weight nuclei: w 2 = 30A -1/ 3 , w 3 = 50A -1/ 3 . 37) For all spherical nuclei the coefficient of vibrational enhancement of the level Kvibr(U') was taken into account according to Eq. 33). 39) where the parameters of the attenuation function are connected with the quadrupole nuclear deformation b by the relations: U r = 120A -1/ 3b2 ; d r = 1400A -2 / 3b2 .

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