Abstract
By comparing the in-plane and out-of-plane orbitally dependent magnetoresistance under a magnetic field of 9 T, the conductive layer thickness of the / interface is determined for temperatures between 45 and 300 K. As the influence of spin-orbit coupling cannot be ignored when considering the conductive layer thickness dependence at temperatures below 45 K, a lower magnetic field is employed. The results show that the thickness increases gradually and then remains constant as the temperature decreases. Such a tendency is well reproduced theoretically by considering the equilibrium between drift and diffusion of electrons near the interface. We discover that the thickness mainly depends on the relative permittivity of and electron mobility, and it is independent of the sheet carrier density. Our investigations show that the dimensionality of the confined zone for electrons can be controlled and can be used as a reference for other interfacial systems in condensed matter physics.
2 More- Received 11 July 2017
- Revised 2 October 2017
DOI:https://doi.org/10.1103/PhysRevB.96.235310
©2017 American Physical Society