Nonlinear spin diffusion and spin rotation in a trapped Fermi gas
arXiv:1501.02677 · doi:10.1103/PhysRevA.91.023614
Abstract
Transverse spin diffusion in a polarized, interacting Fermi gas leads to the Leggett-Rice effect, where the spin current precesses around the local magnetization. With a spin-echo sequence both the transverse diffusivity and the spin-rotation parameter are obtained; the sign of reveals the repulsive or attractive character of the effective interaction. In a trapped Fermi gas the spin diffusion equations become nonlinear, and their numerical solution exhibits an inhomogeneous spin state even at the spin echo time. While the microscopic diffusivity and increase at weak coupling, their apparent values inferred from the trap-averaged magnetization saturate in agreement with a recent experiment for a dilute ultracold Fermi gas.
9 pages, 5 figures; published version
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Cited by in corpus (7)
- Observation of quantum-limited spin transport in strongly interacting two-dimensional Fermi gases
- Universal Spin Transport and Quantum Bounds for Unitary Fermions
- Dynamics of interacting fermions in spin-dependent potentials
- Spin diffusion in ultracold spin-orbit coupled K gas
- Ab initio materials physics and microscopic electrodynamics of media
- A generalized Theory of Diffusion based on Kinetic Theory
- Crossover from collisionless to collisional spin dynamics of polarized fermions