  We study the Fermi surface instabilities of the Pomeranchuk type in the spin
triplet channel with high orbital partial waves ($F_{l}^a ~(l>0)$). The ordered
phases are classified into two classes, dubbed the $\alpha$ and $\beta$-phases
by analogy to the superfluid $^3$He-A and B-phases. The Fermi surfaces in the
$\alpha$-phases exhibit spontaneous anisotropic distortions, while those in the
$\beta$-phases remain circular or spherical with topologically non-trivial spin
configurations in momentum space. In the $\alpha$-phase, the Goldstone modes in
the density channel exhibit anisotropic overdamping. The Goldstone modes in the
spin channel have nearly isotropic underdamped dispersion relation at small
propagating wavevectors. Due to the coupling to the Goldstone modes, the spin
wave spectrum develops resonance peaks in both the $\alpha$ and $\beta$-phases,
which can be detected in inelastic neutron scattering experiments. In the
p-wave channel $\beta$-phase, a chiral ground state inhomogeneity is
spontaneously generated due to a Lifshitz-like instability in the originally
nonchiral systems. Possible experiments to detect these phases are discussed.
