In the ferromagnetic state of an electron gas where the energy bands are spin split, the charge potential produces a spin polarization besides a charge polarization and a magnetic field produces a charge polarization besides a spin polarization. Thus, in a ferromagnetic electron gas, besides the spin susceptibility to a magnetic field χᵐᵐ and the charge susceptibility to a charge potential χᵉᵉ, we introduce two nondiagonal susceptibilities, the spin response to a charge potential χᵐᵉ and the charge response to a magnetic field χᵉᵐ. We present a general formulation for these four susceptibilities and discuss them within the Hartree-Fock or random-phase approximation, taking into account the long-range nature of the Coulomb interaction properly. The importance of the nondiagonal susceptibilities in analyzing observed spin and charge polarization around an impurity is pointed out.
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Kim et al. (1973) studied this question.
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