Spin conductances and spin polarization components in a three-terminal ring subject to Rashba coupling
Source abstract
Abstract
Spin dependent transport in one-dimensional (1D) three-terminal rings is investigated in the presence of the Rashba spin-orbit coupling (RSOC). We focus on the spin dependent conductances and the components of the spin polarization vectors of the currents in the outgoing terminals. For this purpose, the transmission coefficients with respect to the σx, σy and σz basis are obtained, and the three components of the spin polarization vectors are evaluated analytically. The total conductances, the spin dependent conductances and the polarization components are obtained as functions of the incident electron energy, as well as the RSOC strength, for the totally symmetric, partially symmetric and asymmetric cases. It is found that the spin polarizations corresponding to the σy basis are zero, and that there is a symmetry in the total conductances, the spin dependent conductances and the polarization components for symmetric cases, i.e., G1 = G2, g1τ=g2−τ, and P1i=−P2i(i=x,z). This symmetry is attributed to the rotational symmetry in the symmetrically coupled rings. For asymmetric cases, however, it is broken by the asymmetric lead-ring configuration.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Quantum and electron transport phenomena · Molecular Junctions and Nanostructures · Graphene research and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Hebei Normal University 1 College of Physics & Information Engineering and Hebei Advanced Thin Film Laboratory, , Shijiazhuang 050024, People’s Republic of China
Hebei Chemical & Pharmaceutical College 2 , Shijiazhuang 050026, People’s Republic of China
Xingtai Iron and Steel Corporation Limited 3 , Xingtai 054000, People’s Republic of China
Funding
Natural Science Foundation of Hebei Province
References (24)
Show source-provided references
1. Appl. Phys. Lett. · 1990 · 56 · 66510.1063/1.102730 ↗
2. Science · 1998 · 282 · 166010.1126/science.282.5394.1660 ↗
3. Science · 1998 · 294 · 148810.1126/science.1065389 ↗
4. Phys. Rev. · 1959 · 115 · 48510.1103/PhysRev.115.485 ↗
5. Phys. Rev. Lett. · 1984 · 53 · 31910.1103/PhysRevLett.53.319 ↗
6. Appl. Phys. Lett. · 1999 · 75 · 69510.1063/1.124485 ↗
7. Phys. Rev. B · 2004 · 69 · 15533510.1103/PhysRevB.69.155335 ↗
8. Phys. Rev. Lett. · 1986 · 57 · 176110.1103/PhysRevLett.57.1761 ↗
9. Phys. Rev. B · 2005 · 71 · 15532110.1103/PhysRevB.71.155321 ↗
10. Phys. Rev. Lett. · 2005 · 94 · 24660110.1103/PhysRevLett.94.246601 ↗
11. Phys. Rev. B · 2005 · 72 · 07532810.1103/PhysRevB.72.075328 ↗
12. Phys. Rev. B · 2006 · 74 · 11532910.1103/PhysRevB.74.115329 ↗
13. Phys. Rev. B · 2002 · 66 · 07533110.1103/PhysRevB.66.075331 ↗
14. Phys. Rev. B · 2006 · 73 · 15532510.1103/PhysRevB.73.155325 ↗
15. Phys. Rev. B · 2005 · 72 · 23531610.1103/PhysRevB.72.235316 ↗
16. J. Appl. Phys. · 2009 · 105 · 01371010.1063/1.3054322 ↗
17. Ann. Phys. · 2011 · 326 · 110710.1016/j.aop.2010.10.003 ↗
18. J. Appl. Phys. · 2012 · 111 · 04371710.1063/1.3688354 ↗
19. J. Appl. Phys. · 2014 · 116 · 20370310.1063/1.4902847 ↗
20. J. Appl. Phys. · 2013 · 114 · 16431810.1063/1.4827840 ↗
21. Phys. Rev. B · 2004 · 69 · 23531010.1103/PhysRevB.69.235310 ↗
22. Phys. Rev. B · 2002 · 66 · 03310710.1103/PhysRevB.66.033107 ↗
23. Phys. Rev. B · 1992 · 45 · 359310.1103/PhysRevB.45.3593 ↗
24. Phys. Rev. B · 2002 · 65 · 24530710.1103/PhysRevB.65.245307 ↗