Spin transport between polarized Fermi gases near the ferromagnetic phase transition

強磁性相転移近傍の分極フェルミ気体間のスピン輸送

Zhang, T.*; 大上 能悟*; 田島 裕之*; 松尾 衛; Liang, H.*

Zhang, T.*; Oue, Daigo*; Tajima, Hiroyuki*; Matsuo, Mamoru; Liang, H.*

We theoretically study the spin current between two polarized Fermi gases with repulsive interactions near the itinerant ferromagnetic phase transition. We consider a two terminal model where the left reservoir is fixed to be fully polarized while the polarization of the right reservoir is tuned through a fictitious magnetic field defined by the chemical potential difference between different atomic hyperfine states. We calculate the spectra of the spin flip susceptibility function, which displays a magnon dispersion emerging from the Stoner continuum at low momentum in the ferromagnetic phase. Based on the spin flip susceptibility and using Keldysh Green's function formalism, we investigate the spin current induced by quasiparticle and spin flip tunneling processes, respectively, and show their dependence on the polarization bias between two reservoirs. The one body (quasiparticle) tunneling demonstrates a linear dependence with respect to the polarization bias.