Determination of energetic distribution of interface states between gate metal and semiconductor in sub-micron devices from current-voltage characteristics

Density and energetic distributions of interface states between metal-semiconductor rectifying contacts in sub-micron GaAs MESFET and AlGaAs/InGaAs pseudomorphic high electron mobility transistors (HEMT's) have been studied. Electrical properties of the interface states between gate metal and semiconductor in sub-micron devices depend on growth technique, associated processing parameters and surface states on III-V semiconductors. Correlation between nonideal current-voltage (I-V) characteristics and interface states has been established through the bias dependence of ideality factor. Ideality factor determined from I-V characteristics of MESFET and HEMT increases with bias and then decreases after reaching a maximum. A theoretical model based on nonequilibrium approach has been used to determine the density of interface states and their energetic distribution from ideality factor. Essentially, Fermi level shifts with applied bias and Schottky barrier height changes due to trapping and detrapping of electrons by the interface states, and from these changes, density of interface states and their energetic distributions have been determined.

[1]  P. M. Smith,et al.  A 60-GHz high efficiency monolithic power amplifier using 0.1-/spl mu/m PHEMT's , 1995 .

[2]  H. Ikoma,et al.  Nonideal J‐V characteristics and interface states of an a‐Si:H Schottky barrier , 1990 .

[3]  C. Su,et al.  1/f Noise in GaAs MESFETs , 1983, 1983 International Electron Devices Meeting.

[4]  D. Schroder Semiconductor Material and Device Characterization , 1990 .

[5]  V. R. Balakrishnan,et al.  Experimental evidence of surface conduction contributing to transconductance dispersion in GaAs MESFETs , 1997 .

[6]  I. Lindau,et al.  Unified Mechanism for Schottky-Barrier Formation and III-V Oxide Interface States , 1980 .

[7]  H C Card,et al.  Studies of tunnel MOS diodes I. Interface effects in silicon Schottky diodes , 1971 .

[8]  S. Fung,et al.  A systematic approach to the measurement of ideality factor, series resistance, and barrier height for Schottky diodes , 1992 .

[9]  R. Gutmann,et al.  Electrical characteristics of GaAs MIS Schottky diodes , 1979 .

[10]  Ching-Yuan Wu,et al.  A simple interfacial-layer model for the nonideal I-V and C-V characteristics of the Schottky-barrier diode , 1987 .

[11]  Z. Horváth,et al.  Evaluation of the interface state energy distribution from Schottky I‐V characteristics , 1988 .

[12]  J. B. DuBow,et al.  The operation of the semiconductor‐insulator‐semiconductor solar cell: Experiment , 1979 .

[13]  M. Case,et al.  High-efficiency GaAs-based pHEMT C-band power amplifier , 1996 .

[14]  R. Gutmann,et al.  Interface state density in Au-nGaAs Schottky diodes , 1977 .

[15]  D. L. Lile,et al.  The effect of interfacial traps on the stability of insulated gate devices on InP , 1983 .

[16]  M. Shur Physics of Semiconductor Devices , 1969 .

[17]  O. Jantsch,et al.  Flicker (1/f) noise generated by a random walk of electrons in interfaces , 1987, IEEE Transactions on Electron Devices.

[18]  John Bardeen,et al.  Surface States and Rectification at a Metal Semi-Conductor Contact , 1947 .

[19]  Wittmer Conduction mechanism in PtSi/Si Schottky diodes. , 1991, Physical review. B, Condensed matter.

[20]  Hideaki Ikoma,et al.  Current‐voltage characteristics and interface state density of GaAs Schottky barrier , 1993 .

[21]  S.M.Sze,et al.  Surface States and Barrier Height of Metal‐Semiconductor Systems , 1965 .

[22]  I. Lindau,et al.  New and unified model for Schottky barrier and III–V insulator interface states formation , 1979 .

[23]  J. Best The Schottky‐barrier height of Au on n‐Ga1−xAlxAs as a function of AlAs content , 1979 .