Abstract
Properties of magnetic dipole form factors for deformed nuclei are discussed in terms of the angular momentum projected Hartree-Fock-Bogoljubov approximation and the neutron-proton interacting boson model. It is pointed out that there exists a relation between the M1 form factor for the excitation of the orbital K π =1 + band, the M1 form factor for the ground-state band, and the collective M1 form factor in odd- A nuclei.
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