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Abstract:
In order to preserve all the symmetry properties for the effective collective hamiltonian obtained with the generator coordinate method, it is necessary for the trial wave function to have proper transformation properties. The generator coordinates should then transform in the same way as the represented collective operators respectively. And the mass-centre motion should be independent with respect to the internal motion in conformity with the invariance of the nuclear hamiltonian with respect to space rotation and Galilean transformation.
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References
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