SPIN-WAVES IN SPIN-POLARIZED GASES IN THE KNUDSEN REGIME

Boundary conditions are discussed for spin dynamics equations in dilute spinpolarized quantum gases. The bulk equations have the macroscopic "hydrodynamic" form even when mean free paths of the particles are large, and the main question is whether a supplementary "hydrodynamic" boundary condition is valid. Different boundary processes are considered including spin-conserving and non-conserving reflections, slip, formation of adsorbed surface layers, etc. The macroscopic boundary condition fails in the cases of very effective surface processes with violation of time-reversal symmetry (e.g. spin-lattice relaxation) or very high surface-induced diffusion rates. Otherwise, the surface processes are described by a simple boundary condition or by delta-type singularities in bulk equations. The meaning of different macroscopic parameters is clarified. The formation of dense adsorbed boundary layers changes the frequency shifts and linewidths of spin-wave resonance because of effective exchanges between surface and bulk particles and strong interactions within the boundary layers. Here the broadening of resonances is explained not only by additional surface dissipation (diffusion), but also by dephasing processes originating from a renormalization of the molecular field in the boundary layers. The results explain recent experiments by the Cornell group.