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1 ntroduction A description based on rotational, vibrational and smgle par-tiele degrees of freedom has proved to be adequatefor many nuelei. The vibrational modes ean be deseribed either with colleetive variables or as linear combinations of elementary exeitations. Both methods yield the same result in the adiabatic limito The eolleetive and intrinsie degrees of freedom can be mixed through residual terms of the Hamiltonian, sueh as the Coriolis foree and the rotation-vibration interaetion.fatcat:na6kyyylyvaqvmyfye2znfi4ia