SPIN-DEPENDENT CARRIER LOCALIZATION IN FE-BASED SEMIMAGNETIC SEMICONDUCTOR HETEROSTRUCTURES

Citation
Bt. Jonker et al., SPIN-DEPENDENT CARRIER LOCALIZATION IN FE-BASED SEMIMAGNETIC SEMICONDUCTOR HETEROSTRUCTURES, Journal of crystal growth, 159(1-4), 1996, pp. 947-958
Citations number
24
Categorie Soggetti
Crystallography
Journal title
ISSN journal
00220248
Volume
159
Issue
1-4
Year of publication
1996
Pages
947 - 958
Database
ISI
SICI code
0022-0248(1996)159:1-4<947:SCLIFS>2.0.ZU;2-K
Abstract
Semimagnetic (or diluted magnetic) semiconductor heterostructures offe r many unique opportunities for the study of spin dependent effects, i ncluding magnetic field induced quantum confinement and carrier spin l ifetimes, In diluted magnetic semiconductors (DMS) such as Zn1-xFexSe, strong spin exchange interactions significantly modify the band struc ture in the presence of an applied magnetic field. This allows one to continuously and reversibly modify the band offsets in tailored hetero structures to selectively localize carriers according to their spin st ate, thereby providing another degree of freedom in tuning the spatial localization and overlap of carrier wave functions after the fact of growth. We review several examples which have been recently demonstrat ed in Zn1-xFexSe-based heterostructures grown by molecular beam epitax y, including field tunable type-I-type-II transitions, the formation o f a spin superlattice, and the continuous evolution of band alignment to the realization of a re-entrant type-I structure. Additional contro l over carrier confinement and lifetimes via carrier spin is possible in structures which consist of alternating layers of Zn1-xFexSe and Zn 1-yMnySe. In such multiple quantum well systems, the heavy hole excito n simultaneously exhibits both Brillouin and Van Vleck paramagnetic be havior depending upon the spin state probed, Evidence is also observed for the formation of an electron spin population inversion which aris es from the spin splitting of the electron states and the simultaneous spin separation of the holes into different layers of the structure.