TEMPERATURE DISTRIBUTION IN SI-MOSFETS STUDIED BY MICRO RAMAN-SPECTROSCOPY

被引:50
作者
OSTERMEIR, R
BRUNNER, K
ABSTREITER, G
WEBER, W
机构
[1] TECH UNIV MUNICH,WALTER SCHOTTKY INST,W-8046 GARCHING,GERMANY
[2] SIEMENS AG,RES LABS,CORP RES & DEV,W-8000 MUNICH 83,GERMANY
关键词
D O I
10.1109/16.127476
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
The local rise of lattice temperature in n-MOS-FET's is analyzed by the energy shift of the silicon optical phonon using Raman spectroscopy with submicrometer spatial resolution. Operating the devices in saturation a source-drain temperature asymmetry is observed corresponding to the heat dissipation profile that peaks in the pinch-off region. In the substrate surrounding the transistor an anisotropic temperature distribution is found which is related to the geometric shape of the heat source. A reduction of channel length under standard conditions leads to a local temperature increase due to the higher power density. We found temperature increases of less than 20 K for an operating voltage of 5 V for a channel length down to 0.3-mu-m. The experimental results are in good agreement with a model calculation based on idealized device parameters. The time constant of transient heating under pulse operation is determined by analyzing the inhomogeneous broadening of the Raman line. Thermal time constants of about 200 ns are obtained.
引用
收藏
页码:858 / 863
页数:6
相关论文
共 8 条
[1]   ANHARMONIC EFFECTS IN LIGHT-SCATTERING DUE TO OPTICAL PHONONS IN SILICON [J].
BALKANSKI, M ;
WALLIS, RF ;
HARO, E .
PHYSICAL REVIEW B, 1983, 28 (04) :1928-1934
[2]  
CARDONA M, 1975, LIGHT SCATTERING SOL, P4
[3]   RESONANCE RAMAN-SCATTERING IN SI AT ELEVATED-TEMPERATURES [J].
COMPAAN, A ;
TRODAHL, HJ .
PHYSICAL REVIEW B, 1984, 29 (02) :793-801
[4]   CHARACTERISTICS OF A PROPAGATING GAUSSIAN BEAM [J].
DICKSON, LD .
APPLIED OPTICS, 1970, 9 (08) :1854-&
[5]  
MAUTRY PG, ESSDERC 1989, P676
[6]  
Palik E. P., 1985, HDB OPTICAL CONSTANT, P555
[7]  
SMITH DH, 1986, SEMI THERM 86 SCOTTS
[8]  
WHEMPLE SH, 1982, GAAS FET PRINCIPLES