Spin-drag relaxation time in one-dimensional spin-polarized Fermi gases
arXiv:0801.2324 · doi:10.1103/PhysRevB.77.035113
Abstract
Spin propagation in systems of one-dimensional interacting fermions at finite temperature is intrinsically diffusive. The spreading rate of a spin packet is controlled by a transport coefficient termed "spin drag" relaxation time . In this paper we present both numerical and analytical calculations of for a two-component spin-polarized cold Fermi gas trapped inside a tight atomic waveguide. At low temperatures we find an activation law for , in agreement with earlier calculations of Coulomb drag between slightly asymmetric quantum wires, but with a different and much stronger temperature dependence of the prefactor. Our results provide a fundamental input for microscopic time-dependent spin-density functional theory calculations of spin transport in 1D inhomogeneous systems of interacting fermions.
7 pages, 5 figures
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Cited by in corpus (5)
- Spin drag in an ultracold Fermi gas on the verge of a ferromagnetic instability
- Collective excitations in one-dimensional ultracold Fermi gases: a comparative study
- Time-dependent current-density-functional theory of spin-charge separation and spin drag in one-dimensional ultracold Fermi gases
- Spin Drag in Ultracold Fermi Mixtures with Repulsive Interactions
- One-particle spectral function singularities in a one-dimensional gas of spin-1/2 fermions with repulsive delta-function interaction