Schottky and ohmic contacts to doped Si1-x-yGexCy layers

被引:7
作者
Peterson, JJ
Hunt, CE [1 ]
Robinson, M
机构
[1] Univ Calif Davis, Dept Elect & Comp Engn, Davis, CA 95616 USA
[2] Lawrence Semicond Res Lab Inc, Tempe, AZ 85282 USA
关键词
D O I
10.1016/S0038-1101(99)00059-3
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
We report on titanium contacts to n-type and p-type Si1-x-yGexCy strained heteroepitaxial layers on (100)Si and material and electrical characterization of n-type and p-type platinum-silicide-germanide contacts to Si1-x-yGexCy strained heteroepitaxial layers on (100)Si. Ti contacts to n-type Si1-x-yGexCy show rectifying behavior at low doping levels but become ohmic as layers reach 10(18) cm(-3). Ti contacts to p-type Si1-x-yGexCy/Si are ohmic at doping levels as low as 10(15) cm(-3), Contact resistances for Ti/Si1-x-yGexCy contacts had values ranging from 10(-1) to 10(-2) Omega cm(2). X-ray diffraction (XRD) studies of rapid thermal anneal (RTA) silicidation of Pr on SiGeC indicate the reaction proceeds from elemental Pt to Pt-2(SiGeC) and ends in the Pt(SiGeC) phase, analogous to Pt/Si silicides. However, the Pt-silicide-germanide reaction with SiGeC requires higher temperatures than the counterpart Pt reaction with Si. Pt(SiGeC) contacts to n-type SiGeC layers show rectifying behavior with nonideality factors (n) of 1.02 to 1.05 and constant barrier heights of 0.67 eV independent of composition, indicating that Fermi level pinning relative to the SiGeC conduction band is occurring. For contact doping levels of 10(18) cm(-3) and above, Pt(SiGeC) contacts to n-type SiGeC layers are ohmic with constant contact resistance values of 10(-2) Omega cm(2) Pt(SiGeC) contacts to p-type Si1-x-yGexCy/Si were ohmic over the entire doping range studied, with resistances from the 1 Omega cm(2) range at intrinsic alloy doping levels, to the 10(-2) Omega cm(2) range for doping levels of 10(18) cm(-3). Using Pt(SiGeC) ohmic contacts to p-type SiGeC, current-voltage measurements of Si1-x-yGexCy to (100)Si heterojunctions are also presented. Heterojunction barrier heights track the variation of the SiGeC energy bandgap to a factor of 0.84 x. The Si1-x-yGexCy/Si heterojunction valence band discontinuity, Delta E-v, decreases 15 meV per %C incorporated into the strained alloy layer for 0 < y < 0.01 and increases Delta E-v by 2.8 meV per %Ge for 0 < x < 0.11. (C) 1999 Elsevier Science Ltd. All rights reserved.
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页码:1725 / 1734
页数:10
相关论文
共 21 条
[1]   SILICON-BASED SEMICONDUCTOR HETEROSTRUCTURES - COLUMN-IV BANDGAP ENGINEERING [J].
BEAN, JC .
PROCEEDINGS OF THE IEEE, 1992, 80 (04) :571-587
[2]   The effect of carbon on the valence band offset of compressively strained Si1-x-yGexCy/(100) Si heterojunctions [J].
Chang, CL ;
StAmour, A ;
Sturm, JC .
APPLIED PHYSICS LETTERS, 1997, 70 (12) :1557-1559
[3]   ACTIVATION-ENERGY FOR PT2SI AND PTSI FORMATION MEASURED OVER A WIDE-RANGE OF RAMP RATES [J].
COLGAN, EG .
JOURNAL OF MATERIALS RESEARCH, 1995, 10 (08) :1953-1957
[4]   VALENCE-BAND OFFSETS AT STRAINED SI/GE INTERFACES [J].
COLOMBO, L ;
RESTA, R ;
BARONI, S .
PHYSICAL REVIEW B, 1991, 44 (11) :5572-5579
[5]   Co silicide formation on SiGeC/Si and SiGe/Si layers [J].
Donaton, RA ;
Maex, K ;
Vantomme, A ;
Langouche, G ;
Morciaux, Y ;
StAmour, A ;
Sturm, JC .
APPLIED PHYSICS LETTERS, 1997, 70 (10) :1266-1268
[6]   The effect of carbon on strain relaxation and phase formation in the Ti/Si1-x-yGexCy/Si contact system [J].
Eyal, A ;
Brener, R ;
Beserman, R ;
Eizenberg, M ;
Atzmon, Z ;
Smith, DJ ;
Mayer, JW .
APPLIED PHYSICS LETTERS, 1996, 69 (01) :64-66
[7]  
HANAYA H, 1989, JPN J APPL PHYS, V28, pL544
[8]  
JAIN SC, 1994, GERMANIUM SILICON ST, P115
[9]   INTERFACIAL REACTIONS AND SCHOTTKY BARRIERS OF PT AND PD ON EPITAXIAL SI1-XGEX ALLOYS [J].
LIOU, HK ;
WU, X ;
GENNSER, U ;
KESAN, VP ;
IYER, SS ;
TU, KN ;
YANG, ES .
APPLIED PHYSICS LETTERS, 1992, 60 (05) :577-579
[10]  
Mamor M, 1995, MATER RES SOC SYMP P, V379, P137