Optical Manipulation of the Rashba Effect in Germanium Quantum Wells
Source abstract
Abstract
Abstract The Rashba effect in Ge/Si0.15Ge0.85 multiple quantum wells embedded in a p‐i‐n diode is studied through polarization and time‐resolved photoluminescence. In addition to a sizeable redshift arising from the quantum‐confined Stark effect, a threefold enhancement of the circular polarization degree of the direct transition is obtained by increasing the pump power over a 2 kW cm−2 range. This marked variation reflects an efficient modulation of the spin population and is further supported by dedicated investigations of the indirect gap transition. This study demonstrates a viable strategy to engineer the spin‐orbit Hamiltonian through contactless optical excitation and opens the way toward the electro‐optical manipulation of spins in quantum devices based on group‐IV heterostructures.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Quantum and electron transport phenomena · Semiconductor Quantum Structures and Devices · Semiconductor materials and devices
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Universitá degli Studi di Milano‐Bicocca Dipartimento di Scienza dei Materiali LNESS and BiQuTe, Via R. Cozzi 55 Milan 20125 Italy
LNESS and Dipartimento di Fisica del Politecnico di Milano Polo di Como Via Anzani 42 Como I‐22100 Italy
Universitá degli Studi di Milano‐Bicocca Dipartimento di Scienza dei Materiali MIBSOLAR, Via R. Cozzi 55 Milan 20125 Italy
Université de Toulouse INSA‐CNRS‐UPS, LPCNO, 135 Ave. de Rangueil Toulouse 31077 France
References (43)
Show source-provided references
1. 10.1016/0375-9601(71)90196-410.1016/0375-9601(71)90196-4 ↗
2. Ivchenko E. · JETP Lett. · 1978 · 27 · 604
3. 10.1016/0038-1098(90)90963-C10.1016/0038-1098(90)90963-C ↗
4. 10.1007/978-3-319-65436-210.1007/978-3-319-65436-2 ↗
5. Rashba E. I. · Fiz. Tverd. Tela: Collect. Pap. · 1959 · 2 · 162
6. 10.1088/0022-3719/17/33/01510.1088/0022-3719/17/33/015 ↗
7. 10.1103/PhysRevB.82.04531710.1103/PhysRevB.82.045317 ↗
8. 10.1103/PhysRevLett.77.182910.1103/PhysRevLett.77.1829 ↗
9. 10.1103/PhysRevLett.107.13660410.1103/PhysRevLett.107.136604 ↗
10. 10.1103/RevModPhys.89.01100110.1103/RevModPhys.89.011001 ↗
11. 10.1038/ncomms1388610.1038/ncomms13886 ↗
12. 10.1038/nature0420410.1038/nature04204 ↗
13. 10.1088/0953-8984/18/3/01810.1088/0953-8984/18/3/018 ↗
14. 10.1063/1.477431610.1063/1.4774316 ↗
15. 10.1103/PhysRevLett.113.08660110.1103/PhysRevLett.113.086601 ↗
16. 10.1063/1.490110710.1063/1.4901107 ↗
17. 10.1103/PhysRevLett.108.15660310.1103/PhysRevLett.108.156603 ↗
18. 10.1103/PhysRevB.85.24130310.1103/PhysRevB.85.241303 ↗
19. 10.1023/A:102368041235010.1023/A:1023680412350 ↗
20. 10.1103/PhysRevLett.98.18720310.1103/PhysRevLett.98.187203 ↗
21. 10.3390/electronics601001910.3390/electronics6010019 ↗
22. 10.15407/spqeo12.04.33910.15407/spqeo12.04.339 ↗
23. 10.1109/TED.2007.90287110.1109/TED.2007.902871 ↗
24. 10.1103/PhysRevB.78.04140710.1103/PhysRevB.78.041407 ↗
25. 10.1063/1.310662110.1063/1.3106621 ↗
26. 10.1103/PhysRevLett.110.17740410.1103/PhysRevLett.110.177404 ↗
27. 10.1088/0268-1242/30/10/10500110.1088/0268-1242/30/10/105001 ↗
28. 10.1063/1.367327110.1063/1.3673271 ↗
29. 10.1103/PhysRevB.54.1638910.1103/PhysRevB.54.16389 ↗
30. 10.1103/PhysRevLett.53.217310.1103/PhysRevLett.53.2173 ↗
31. 10.1038/nphoton.2014.7310.1038/nphoton.2014.73 ↗
32. 10.1364/OL.37.00396010.1364/OL.37.003960 ↗
33. 10.1063/1.364757210.1063/1.3647572 ↗
34. 10.1103/PhysRevB.77.16531510.1103/PhysRevB.77.165315 ↗
35. 10.1103/PhysRevB.84.12532310.1103/PhysRevB.84.125323 ↗
36. 10.1103/PhysRevB.80.20530910.1103/PhysRevB.80.205309 ↗
37. 10.1103/PhysRevB.20.328510.1103/PhysRevB.20.3285 ↗
38. 10.1016/0038-1101(78)90216-210.1016/0038-1101(78)90216-2 ↗
39. 10.1103/PhysRevB.86.08520210.1103/PhysRevB.86.085202 ↗
40. 10.1002/pssb.20135026110.1002/pssb.201350261 ↗
41. 10.1116/1.58142210.1116/1.581422 ↗
42. 10.1038/s41598-018-29409-310.1038/s41598-018-29409-3 ↗
43. 10.1103/PhysRevB.88.04520410.1103/PhysRevB.88.045204 ↗