  We study the indirect exchange interaction between two localized magnetic
moments, known as Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction, in a
one-dimensional spin-polarized electron gas. We find explicit expressions for
each term of this interaction, study their oscillatory behaviors as a function
of the distance between two magnetic moments, $R$, and compare them with the
known results for RKKY interaction in the case of one-dimensional standard
electron gas. We show this interaction can be written in an anisotropic
Heisenberg form, $E(\vec
R)=\lambda^2\chi_{xx}(S_{1x}S_{2x}+S_{1y}S_{2y})+\lambda^2\chi_{zz}\,
S_{1z}S_{2z}$, coming from broken time-reversal symmetry of the host material.
