Photoionization cross-section of the DX center in Te-doped AlxGa1-xSb

被引:9
作者
Baraldi, A [1 ]
Ghezzi, C [1 ]
Magnanini, R [1 ]
Parisini, A [1 ]
Tarricone, L [1 ]
Zerbini, S [1 ]
机构
[1] Univ Parma, Ist Nazl Fis Mat, Dipartimento Fis, I-43100 Parma, Italy
关键词
D O I
10.1063/1.366720
中图分类号
O59 [应用物理学];
学科分类号
摘要
The photoionization of DX centers in Te-doped AlxGa1-xSb layers grown by molecular beam epitaxy is investigated by measuring the increase of the Hall free electron density after illumination by monochromatic light in the temperature range typical of the persistent photoconductivity (PPC) effect. The investigated samples have AlSb molar fractions in the 0.3 less than or equal to x less than or equal to 0.5 range and n-type doping in the 10(17)-10(18) cm(-3) range. An accurate investigation of the isothermal photoionization transients is performed to evidence features in the curve not directly related to the phenomenology of the DX center, the free electron density being influenced by the possible occupancy of other impurity levels. The transients show, in particular, an initial nonexponential behavior which is demonstrated as due to localization of a fraction of the photoexcited electrons into a nonmetastable impurity state which is responsible for the semiconductor-to-metal transition observed under the PPC regime. When this effect is accounted for, the dependence of the photoionization cross section of the DX center on the photon energy was obtained from the analysis of the linear part of the transients and analyzed through a model given in the literature. The analysis gives values of the optical ionization energy and of the Frank-Condon shift varying in the ranges of 0.84-0.95 and 0.70-0.74 eV, respectively, depending on the alloy composition. This confirms a large lattice relaxation for the DX center related to the Te-impurity in AlxGa1-xSb. (C) 1998 American Institute of Physics.
引用
收藏
页码:491 / 496
页数:6
相关论文
共 23 条
[1]   Electron mobility and physical magnetoresistance in n-type GaSb layers grown by molecular beam epitaxy [J].
Baraldi, A ;
Colonna, F ;
Ghezzi, C ;
Magnanini, R ;
Parisini, A ;
Tarricone, L ;
Bosacchi, A ;
Franchi, S .
SEMICONDUCTOR SCIENCE AND TECHNOLOGY, 1996, 11 (11) :1656-1667
[2]   Control of the n-type doping in AlxGa1-xSb: DX-center behavior of the Te impurity [J].
Baraldi, A ;
Colonna, F ;
Covucci, G ;
Ghezzi, C ;
Magnanini, R ;
Parisini, A ;
Tarricone, L ;
Bosacchi, A ;
Franchi, S .
MATERIALS SCIENCE AND ENGINEERING B-SOLID STATE MATERIALS FOR ADVANCED TECHNOLOGY, 1997, 44 (1-3) :70-73
[3]   Coexistence of the DX center with nonmetastable states of the donor impurity in Si-doped AlxGa1-xAs: Effects on the low-temperature electron mobility [J].
Baraldi, A ;
Frigeri, P ;
Ghezzi, C ;
Parisini, A ;
Bosacchi, A ;
Franchi, S ;
Gombia, E ;
Mosca, R .
PHYSICAL REVIEW B, 1996, 53 (16) :10715-10727
[4]   LOW-TEMPERATURE OCCUPATION OF A DONOR STATE RESONANT WITH THE CONDUCTION-BAND IN AL0.35GA0.65AS [J].
BARALDI, A ;
COLONNA, E ;
FRIGERI, P ;
GHEZZI, C ;
PARISINI, A ;
GOMBIA, E ;
MOSCA, R .
PHYSICAL REVIEW B, 1993, 48 (24) :17835-17840
[5]  
BOURGOIN C, 1989, SOLID STATE PHENOMEN, V10
[6]   CHARACTERIZATION OF TE-DOPED GASB GROWN BY MOLECULAR-BEAM EPITAXY USING SNTE [J].
CHEN, JF ;
CHO, AY .
JOURNAL OF APPLIED PHYSICS, 1991, 70 (01) :277-281
[7]   EVIDENCE FOR SUBSTITUTIONAL-INTERSTITIAL DEFECT MOTION LEADING TO DX BEHAVIOR BY DONORS IN ALXGA1-XAS [J].
DOBACZEWSKI, L ;
KACZOR, P ;
MISSOUS, M ;
PEAKER, AR ;
ZYTKIEWICZ, ZR .
PHYSICAL REVIEW LETTERS, 1992, 68 (16) :2508-2511
[8]   WAVE-FUNCTIONS AND OPTICAL CROSS-SECTIONS ASSOCIATED WITH DEEP CENTERS IN SEMICONDUCTORS [J].
JAROS, M .
PHYSICAL REVIEW B, 1977, 16 (08) :3694-3706
[9]   TRAPPING CHARACTERISTICS AND A DONOR-COMPLEX (DX) MODEL FOR THE PERSISTENT PHOTOCONDUCTIVITY TRAPPING CENTER IN TE-DOPED ALXGA1-XAS [J].
LANG, DV ;
LOGAN, RA ;
JAROS, M .
PHYSICAL REVIEW B, 1979, 19 (02) :1015-1030
[10]   PHOTOIONIZATION CROSS-SECTION OF THE DX CENTER IN SI-DOPED ALXGA1-XAS [J].
LEGROS, R ;
MOONEY, PM ;
WRIGHT, SL .
PHYSICAL REVIEW B, 1987, 35 (14) :7505-7510