2016
DOI: 10.1007/s10773-015-2908-4
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Thermal Bias on the Pumped Spin-Current in a Two-Level Quantum Dot

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“…The pure spin current has been implemented successfully through the spin Hall effect, [22][23][24][25] nonlocal spin valves, 10,19,26 spin pumping, [27][28][29][30] magnetization dynamics, 31 the longitudinal spin Seebeck effect, [32][33][34][35] and nonlocal spin injection. 18,36,37 Various new mechanisms are also developed to generate the pure spin current, for example, the adiabatic twisting of a magnetic molecule in graphene, 38 Auger recombination in Rashba quantum wells 39 with Rashba SOC, and the separation of the chiral states with perfect spin polarization in two-dimensional honeycomb lattices.…”
Section: Introductionmentioning
confidence: 99%
“…The pure spin current has been implemented successfully through the spin Hall effect, [22][23][24][25] nonlocal spin valves, 10,19,26 spin pumping, [27][28][29][30] magnetization dynamics, 31 the longitudinal spin Seebeck effect, [32][33][34][35] and nonlocal spin injection. 18,36,37 Various new mechanisms are also developed to generate the pure spin current, for example, the adiabatic twisting of a magnetic molecule in graphene, 38 Auger recombination in Rashba quantum wells 39 with Rashba SOC, and the separation of the chiral states with perfect spin polarization in two-dimensional honeycomb lattices.…”
Section: Introductionmentioning
confidence: 99%