Electromagnetic form factors of odd-Aaxially symmetric deformed nuclei

Expressions for electron scattering form factors for odd-$A$ deformed nuclei are derived by projecting states with definite angular momentum from an axially symmetric intrinsic wave function. Through an expansion of the multipole matrix elements in terms of $\frac{1}{〈{J_y}^2〉}$ both single-particle and collective contributions are taken into account in a systematic way. Selection rules are discussed and some schematic calculations of magnetic form factors are presented for ${}_{}{}^{25}{}_{}{}^{}\mathrm{Mg}$ and ${}_{}{}^{181}{}_{}{}^{}\mathrm{Ta}$.