RBS study of annealing effects in passivated mercury cadmium telluride

被引:2
作者
Anjali [1 ]
Srivastava, P
Mohapatra, S
Lenka, HP
Pal, R
Vyas, HP
Sekhar, BR
Sehgal, HK
机构
[1] Indian Inst Technol, Dept Phys, New Delhi 110016, India
[2] Inst Phys, Bhubaneswar 751005, Orissa, India
[3] Solid State Phys Lab, Delhi 110054, India
关键词
D O I
10.1088/0268-1242/20/10/015
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Changes in composition in passivated mercury cadmium telluride (Hg1-xCdXTe or MCT) due to annealing have been investigated using Rutherford backscattering spectroscopy (RBS). Different passivated structures such as anodic oxide/MCT, CdTe/MCT and ZnS/MCT annealed at 80 degrees C in 10(-6) Torr (parameters used during device packaging) have been studied and compared with the as-deposited samples. It is found that in as-deposited samples of anodic oxide/MCT and ZnS/MCT, the interface between the passivating layer and the MCT substrate is very sharp and composition of the capping layer remains constant throughout. Composition of the anodic oxide layer is estimated to be Hg:Te:Cd:O::0.4:1:0.25:3.35 while that of ZnS is Zn:S::0.9:1.1. In an annealed anodic oxide/MCT sample, the composition of the upper layer is different from that in the as-deposited sample and the interface is comparatively wider, while in the annealed ZnS/MCT sample the thickness of the interfacial region is found to be more than 50 nm and the composition of the remaining ZnS layer remains unaltered. The composition of the CdTe layer in both cases (as-deposited and annealed) is Cd:Te::l:l and the interface thickness of the as-deposited sample is found to be similar to 35 nm; which on annealing, increases to similar to 50 nm.
引用
收藏
页码:1072 / 1077
页数:6
相关论文
共 14 条
[1]   CdTe and anodic oxides on Hg1-xCdxTe:: interface and compositional analysis using Rutherford backscattering spectroscopy [J].
Anjali, PS ;
Mohapatra, S ;
Pal, R ;
Vyas, HP ;
Sekhar, BR ;
Sehgal, HK .
SURFACE AND INTERFACE ANALYSIS, 2005, 37 (06) :562-567
[2]   ANODIC OXIDE COMPOSITION AND HG DEPLETION AT THE OXIDE-SEMICONDUCTOR INTERFACE OF HG1-XCDXTE [J].
DAVIS, GD ;
SUN, TS ;
BUCHNER, SP ;
BYER, NE .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY, 1981, 19 (03) :472-476
[3]  
DORNHAUS R, 1983, SPRINGER TRACTS MODE, V98, P138
[4]   RAMAN ANALYSIS OF ANODIC FILMS ON MERCURY CADMIUM TELLURIDE [J].
HILL, IR ;
CHANG, WH ;
LAU, WM .
JOURNAL OF APPLIED PHYSICS, 1990, 68 (11) :5621-5624
[5]   Bake stability of CdTe and ZnS on HgCdTe: An x-ray photoelectron spectroscopy study [J].
Jha, SK ;
Srivastava, P ;
Pal, R ;
Anjali ;
Sehgal, HK ;
Lee, HC ;
Agnihotri, OP ;
Gong, BB .
JOURNAL OF ELECTRONIC MATERIALS, 2003, 32 (08) :899-905
[6]   THERMAL-STABILITY OF OXIDE-FILMS ON CD0.2 HG0.8 TE - A COMBINED SIMS, AES, AND XPS STUDY [J].
KAISER, U ;
GANSCHOW, O ;
WIEDMANN, L ;
BENNINGHOVEN, A .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY A-VACUUM SURFACES AND FILMS, 1983, 1 (02) :657-661
[7]  
PAL R, 2003, Patent No. 13782003
[8]   PROPERTIES OF INSULATOR INTERFACES WITH PARA-HGCDTE [J].
SCHACHAM, SE ;
FINKMAN, E .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY A-VACUUM SURFACES AND FILMS, 1990, 8 (02) :1171-1173
[9]   INTERFACE PROPERTIES OF VARIOUS PASSIVATIONS OF HGCDTE [J].
SCHACHAM, SE ;
FINKMAN, E .
OPTICAL ENGINEERING, 1990, 29 (07) :795-799
[10]   QUANTITATIVE MEASUREMENTS OF THE STOICHIOMETRY OF ANODIC OXIDES GROWN ON HG0.78CD0.22 TE [J].
STAHLE, CM ;
THOMSON, DJ ;
HELMS, CR ;
BECKER, CH ;
SIMMONS, A .
APPLIED PHYSICS LETTERS, 1985, 47 (05) :521-523