A field theory describing the low-energy, long-wavelength sector of an
incommensurate, spiral magnetic phase is derived from a spin-fermion
model that is commonly used as a microscopic model for high-temperatur
e superconductors. After integrating out the fermions in a path-integr
al representation, a gradient expansion of the fermionic determinant i
s performed. This leads to an O(3)xO(2)-symmetric quantum nonlinear si
gma model, where the doping dependence is explicitly given by generali
zed fermionic susceptibilities which enter into the coupling constants
of the sigma model and contain the fermionic band-structure that resu
lts from the spiral background. A stability condition of the field the
ory self-consistently determines the spiral wavevector as a function o
f the doping concentration. Furthermore, terms of topological nature l
ike the theta-vacuum term in (1+1)-dimensional nonlinear a models are
obtained for the plane of the spiral.