Optical gain and laser emission in HgCdTe heterostructures

被引:18
作者
BonnetGamard, J
Bleuse, J
Magnea, N
Pautrat, JL
机构
[1] CEA/Département de Recherche, Fondamentale Sur la Matière Condensée, CENG 17, F-38054 Grenoble Cedex 9, rue des Martyrs
关键词
D O I
10.1063/1.360457
中图分类号
O59 [应用物理学];
学科分类号
摘要
A detailed study of stimulated emission mechanisms as well as laser emission capability has been carried out on Hg1-xCdxTe (0.44<x<0.5) separate-confinement heterostructures grown by molecular beam epitaxy. At low temperature, spontaneous photoluminescence (PL) occurs on extrinsic levels below the gap whereas optical gain exhibits a maximum of stimulated emission shifted towards higher energy, close to the gap. As temperature increases, spontaneous PL is shifted from the extrinsic states to the band-to-band transition by a thermally activated detrapping of the carriers. Above 100 K, spontaneous and stimulated emission vary in a similar way with temperature. Laser emission has been observed up to room temperature for all the heterostructures. The use of quantum wells in the active layer and graded index in the barriers has allowed a significant reduction of the excitation density threshold, as compared to a single separate-confinement heterostructure (SCH) of same composition. However, the high-temperature characteristic temperature T-0 is found to be similar in the two structures. A SCH with a higher energy gap exhibits a more favorable behavior with temperature. These experimental results have been compared to theoretical models. The experimentally observed T-0 can be well simulated by taking into account the Auger effect. From the experimental data, the Auger constant has been determined for each heterostructure. (C) 1995 American Institute of Physics.
引用
收藏
页码:6908 / 6915
页数:8
相关论文
共 30 条
[1]  
Agrawal G., 1986, LONG WAVELENGTH SEMI
[2]   HGCDTE INFRARED DIODE-LASERS GROWN BY MBE [J].
ARIAS, JM ;
ZANDIAN, M ;
ZUCCA, R ;
SINGH, J .
SEMICONDUCTOR SCIENCE AND TECHNOLOGY, 1993, 8 (01) :S255-S260
[3]  
BEBB HB, 1972, SEMICONDUCT SEMIMET, V8, pCH4
[4]   ROOM-TEMPERATURE LASER-EMISSION NEAR 2 MU-M FROM AN OPTICALLY PUMPED HGCDTE SEPARATE-CONFINEMENT HETEROSTRUCTURE [J].
BLEUSE, J ;
MAGNEA, N ;
ULMER, L ;
PAUTRAT, JL ;
MARIETTE, H .
JOURNAL OF CRYSTAL GROWTH, 1992, 117 (1-4) :1046-1049
[5]   MESA STRIPE TRANSVERSE INJECTION-LASER IN HGCDTE [J].
BOUCHUT, P ;
DESTEFANIS, G ;
BABLET, J ;
MILLION, A ;
COLIN, T ;
RAVETTO, M .
APPLIED PHYSICS LETTERS, 1992, 61 (13) :1561-1563
[6]  
BRICE J, 1989, EMIS DATA REV SERI B, V14, P113
[7]   THEORETICAL GAIN IN STRAINED INGAAS/ALGAAS QUANTUM-WELLS INCLUDING VALENCE-BAND MIXING EFFECTS [J].
CORZINE, SW ;
YAN, RH ;
COLDREN, LA .
APPLIED PHYSICS LETTERS, 1990, 57 (26) :2835-2837
[8]   STIMULATED-EMISSION AT 2.8-MU-M FROM HG-BASED QUANTUM WELL STRUCTURES GROWN BY PHOTOASSISTED MOLECULAR-BEAM EPITAXY [J].
GILES, NC ;
HAN, JW ;
COOK, JW ;
SCHETZINA, JF .
APPLIED PHYSICS LETTERS, 1989, 55 (19) :2026-2028
[9]   BAND-TO-BAND AUGER RECOMBINATION IN SEMICONDUCTORS [J].
HAUG, A .
JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS, 1988, 49 (06) :599-605
[10]  
Horikoshi Y., 1985, SEMICONDUCTORS SEM C, V22C