Higher Chern number states in curved periodic nanowires
Source abstract
Abstract
Abstract The coupling between the spin and momentum degrees of freedom due to spin–orbit interactions (SOI) suggests that the strength of the latter can be modified by controlling the motion of the charge carriers. In this paper, we investigate how the effective SOI can be modulated by constraining the motion of charge carriers to curved waveguides thereby introducing real-space geometric curvature in their motion. The change in the SOI can in turn induce topological phase transitions in the system. Specifically, we study how the introduction of periodic sinusoidal curvature in nanowires with intrinsic SOC can induce the onset of mid-gap topologically protected edge states, which can be characterized by a topological invariant or Chern number. The Chern number corresponds to the number of discrete charges that would be pumped across the length of the nanowire when the phase of a sliding gate potential relative to that of the sinusoidal curvature is varied adiabatically over a complete period. In addition, coupling to an external magnetization can be utilized as an experimental knob to modify the Chern number by displacing the energies of the curvature-induced bands relative to one another. The magnetization can be tuned to achieve large discrete jumps in the number of pump charges per phase period.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Topological Materials and Phenomena · Quantum and electron transport phenomena · Quantum many-body systems
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (43)
Show source-provided references
1. Geometrical effect on spin transport10.1142/S2010324713400067 ↗
2. Curvature-induced spin–orbit coipling and spin relaxation in a chemically clean single-layer graphene10.1103/PhysRevB.84.195457 ↗
3. One-dimensional ring in the presence of rashba spin–orbit interaction: derivation of the correct Hamiltonian10.1103/PhysRevB.66.033107 ↗
4. Exact hamiltonians with rashba and cubic dresselhaus spin–orbit couplings on a curved surface10.1103/PhysRevB.87.174413 ↗
5. Designing electron spin textures and spin interferometers by shape deformations10.1103/PhysRevB.94.081406 ↗
6. Spin precession and modulation in ballistic cylindrical nanowires due to the Rashba effect10.1103/PhysRevB.83.115305 ↗
7. Geometrical effect on the non-Abelian spin–orbital gauge field of a curved surface10.1103/PhysRevB.84.214423 ↗
8. Spin and charge transport in U-shaped one-dimensional channels with spin–orbit couplings10.1103/PhysRevB.84.085307 ↗
9. Quantum transport in a curved one-dimensional quantum wire with spin-orbit interactions10.1103/PhysRevB.75.085308 ↗
10. Semicircular Rashba arc spin polarizer10.1063/1.4866388 ↗
11. Indepdent geometrical control of spin and charge resistances in curved spintronics10.1021/acs.nanolett.9b01994 ↗
12. Geometric effects in the electronic transport of deformed nanotubes10.1088/0957-4484/27/13/135302 ↗
13. Geometric effects of a quarter of corrugated torus10.3390/condmat4010003 ↗
14. The geometric potential of a double-frequency corrugated surface10.1016/j.physleta.2019.04.013 ↗
15. Transmission gaps from corrugations10.1088/0022-3727/49/29/295103 ↗
16. Tuning the electrical resistivity of semiconductor thin films by nanoscale corrugation10.1103/PhysRevB.79.235407 ↗
17. Curvature induced out-of-plane spin accumulation in Rashba quantum waveguides10.1063/1.4986485 ↗
18. Quantum spin Hall effect and topological phase transition in HgTe quantum wells10.1126/science.1133734 ↗
19. Quantum spin Hall insulator state in HgTe quantum wells10.1126/science.1148047 ↗
20. Quantized Hall conductance in a two-dimensional periodic potential10.1103/PhysRevLett.49.405 ↗
21. Z2 topological order and the quantum spin Hall effect10.1103/PhysRevLett.95.146802 ↗
22. Colloquium: topological insulators10.1103/RevModPhys.82.3045 ↗
23. The birth of topological insulators10.1038/nature08916 ↗
24. Topological insualtors and superconductors10.1103/RevModPhys.83.1057 ↗
25. Curvature induced quantum phase transitions in an electron-hole system10.1038/s41598-018-34903-9 ↗
26. Edge states and topologicial insulating phases generatred by curving a nanowire with RSOC10.1103/PhysRevLett.115.256801 ↗
27. Topologcial qunatum pump in serpentine-shaped semiconducting narrow channels10.1103/PhysRevB.97.241103 ↗
28. Topologcial two-parameter charge pump in a one-dimensional semiconductor nanowire superlattice10.1103/PhysRevB.100.075402 ↗
29. Gauge fields in spintronics10.1063/1.3665219 ↗
30. Yang–Mills physics in Spintronics10.1016/j.physrep.2020.08.002 ↗
31. Experimental demonstration of spin geometric phase: radius dependence of time-reversal Aharonov–Casher oscillations10.1103/PhysRevLett.108.086801 ↗
32. Aharonov–Bohm rings with strong spin–orbit interaction: the role of sample-specific properties10.1088/1367-2630/15/3/033029 ↗
33. Engineered spin–orbit interactions in LaAlO3/SrTiO3-based 1D serpentine electron waveguides10.1126/sciadv.aba6337 ↗
34. Tunable spin and orbital polarization in SrTiO3-based heterostructures10.1088/1367-2630/ab4735 ↗
35. Quantum mecahnics of a constrained particle10.1103/PhysRevA.23.1982 ↗
36. Quantum mechanics with constraints10.1016/0003-4916(71)90031-5 ↗
37. Inherent orbital spin textures in Rashba effect and their implications in spin-orbitronics10.1088/1361-648X/aac86f ↗
38. Gate control of spin-oribit interaction in an inverted In0.53Ga0.47As/In0.52Al0.48As heterostructure10.1103/PhysRevLett.78.1335 ↗
39. Effects of inversion asymmetry on electron energy band structures in GaSb/InAs/GaSb quantum wells10.1103/PhysRevB.41.7685 ↗
40. Z2 classification of quantum spin Hall systems: an approach using time-reversal invariance10.1103/PhysRevB.79.195321 ↗
41. Quantum anomalous Hall effect in topological insulator memory10.1063/1.4916999 ↗
42. Topological insulator cell for memory and magnetic sensor applications10.1143/APEX.4.094201 ↗
43. Robustness of topological hall effect of nontrivial spin textures10.1038/srep05123 ↗