  We derive the exact ground states for a one dimensional family of $S=1/2$ XXZ
Hamiltonians on the zigzag ladder. These states exhibit true long range spiral
order that spontaneously breaks the U(1) invariance of the Hamiltonian. Besides
breaking a continuous symmetry in $d=1$, this spiral ordering has a
ferromagnetic component along the symmetry axis that can take any value between
zero and full saturation. In this sense, our canted spiral solutions are a
generalization of the SU(2) Heisenberg ferromagnet to non-zero ordering
wave-vectors of the transverse spin components. We extend this result to the
$d=2$ anisotropic triangular lattice.
