Indirect barrier electron-hole gas transitions in mixed type-I-type-II GaAs/AlAs multiple quantum wells - art. no. 035314

Citation
R. Guliamov et al., Indirect barrier electron-hole gas transitions in mixed type-I-type-II GaAs/AlAs multiple quantum wells - art. no. 035314, PHYS REV B, 6403(3), 2001, pp. 5314
Citations number
18
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
6403
Issue
3
Year of publication
2001
Database
ISI
SICI code
0163-1829(20010715)6403:3<5314:IBEGTI>2.0.ZU;2-4
Abstract
We studied the photoluminescence (PL) spectrum resulting of the indirect re combination of barrier electrons and the two-dimensional hole gas (2DHG) th at is excited in a structure of mixed type-I-type-II GaAs/AIAs quantum well s. This structure consists of alternating narrow and wide GaAs quantum well s (QW), and is distinguished by a staggered conduction-band alignment that leads to a fast electron transfer from the narrow to the wide QW's and a ve ry slow hole transfer. Consequently, a 2DHG and a two-dimensional electron gas (2DEG) are formed in the narrow and wide QW's, respectively. Their dens ity is controlled by the photoexcitation intensity and is experimentally de termined by fitting the band shape of the wide-well direct-recombination PL spectra (in the range of 10(10)<n(e)<5 x 10(11) cm(-2)). A small fraction of the electrons recombine radiatively with the 2DHG while they are in the lowest X subband of the AlAs barrier, and the resulting spectrum is investi gated at T=2 K and for various excitation intensities. The indirect transit ions consist of a no-phonon band and momentum conserving (zone-edge) phonon sidebands. All these bands are blueshifted with increasing photoexcitation intensity. This shift is well explained by calculating the lowest X subban d energy in the electrostatic potential, generated by the separate 2DEG and 2DHG charges as a function of their density.