TY - JOUR
T1 - Symmetry and transport property of spin current induced spin-Hall effect
AU - Xing, Yanxia
AU - Sun, Qing Feng
AU - Wang, Jian
PY - 2007/2/15
Y1 - 2007/2/15
N2 - We study the spin current induced spin-Hall effect that a longitudinal spin-dependent chemical potential q Vs=x,y,z induces transverse spin conductances Gs s′. A four-terminal system with the Rashba and Dresselhaus spin-orbit interactions (SOIs) in the scattering region is considered. By using Landauer-Büttiker formula with the aid of Green's function, various spin current induced spin-Hall conductances Gs s′ are calculated. With the charge chemical potential q Vc or spin chemical potential q Vs=x,y,z, there are 16 elements for the transverse conductances Gp μν = Jp,μ Vν, where μ,ν=x,y,z,c. Due to the symmetry of our system, these elements are not independent. For the system with C2 symmetry half of the elements are zero when only the Rashba SOI or the Dresselhaus SOI exists in the center region. The numerical results show that of all the conductance elements, the spin current induced spin-Hall conductances Gs s′ are usually much greater (about one or two orders of magnitude) than the spin-Hall conductances Gsc and the reciprocal spin-Hall conductances Gcs. So the spin current induced spin-Hall effect dominates in the present device.
AB - We study the spin current induced spin-Hall effect that a longitudinal spin-dependent chemical potential q Vs=x,y,z induces transverse spin conductances Gs s′. A four-terminal system with the Rashba and Dresselhaus spin-orbit interactions (SOIs) in the scattering region is considered. By using Landauer-Büttiker formula with the aid of Green's function, various spin current induced spin-Hall conductances Gs s′ are calculated. With the charge chemical potential q Vc or spin chemical potential q Vs=x,y,z, there are 16 elements for the transverse conductances Gp μν = Jp,μ Vν, where μ,ν=x,y,z,c. Due to the symmetry of our system, these elements are not independent. For the system with C2 symmetry half of the elements are zero when only the Rashba SOI or the Dresselhaus SOI exists in the center region. The numerical results show that of all the conductance elements, the spin current induced spin-Hall conductances Gs s′ are usually much greater (about one or two orders of magnitude) than the spin-Hall conductances Gsc and the reciprocal spin-Hall conductances Gcs. So the spin current induced spin-Hall effect dominates in the present device.
UR - http://www.scopus.com/inward/record.url?scp=33847009140&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.75.075324
DO - 10.1103/PhysRevB.75.075324
M3 - Article
AN - SCOPUS:33847009140
SN - 1098-0121
VL - 75
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 7
M1 - 075324
ER -