Investigation of cross-sectional potential distribution in GaN-based field effect transistors by Kelvin probe force microscopy

Cross-sectional potential distribution of AlGaN/GaN HFETs with and without surface passivation by silicon nitride (SiNx) has been investigated by using Kelvin probe force microscopy to study the effect of the surface passivation layer on an electric field under high operating bias conditions. The measured FETs exhibited DC characteristics of the maximum drain current of 750 mA/mm, threshold voltage of -5 V, and the transconductance of 150 mS/mm. For the bias condition of the gate voltage of -5 V and the drain voltage of 40 V, the electric field is mainly concentrated at three areas without relation to the presence or absence of the surface passivation layer. One is the mid-point between the gate and drain electrodes at FET surface. The others are the mid-depth of GaN buffer layer under the drain electrode and the interface between GaN buffer and SiC substrates from drain edge toward source electrode. Near the surface of SiNx-passivated AlGaN/GaN HFETs, it is confirmed that the intensity of electric field concentration decreases compared to that of no-passivated AlGaN/GaN HFETs. It is considered that this result originates in the decrease of the surface charge by SiNx passivation. In addition, It is found that the electric field concentration near the GaN/SiC interface has a tendency to become stronger rather than that between the drain and gate electrodes by SiNx passivation.

[1]  H. K. Wickramasinghe,et al.  Kelvin probe force microscopy , 1991 .

[2]  O. Vatel,et al.  Kelvin probe force microscopy for potential distribution measurement of semiconductor devices , 1995 .

[3]  M. Arakawa,et al.  Kelvin Probe Force Microscopy for Potential Distribution Measurement of Cleaved Surface of GaAs Devices , 1996 .

[4]  M. Arakawa,et al.  Kelvin Probe Force Microscopy for Potential Distribution Measurement of Cleaved Surface of GaAs Devices , 1996 .

[5]  A. Stemmer,et al.  Resolution and contrast in Kelvin probe force microscopy , 1998 .

[6]  Edward T. Yu,et al.  Gate leakage current mechanisms in AlGaN/GaN heterostructure field-effect transistors , 2000 .

[7]  Michael G. Spencer,et al.  Surface potential measurements on GaN and AlGaN/GaN heterostructures by scanning Kelvin probe microscopy , 2001 .

[8]  U. Mishra,et al.  AlGaN/GaN HEMTs-an overview of device operation and applications , 2002, Proc. IEEE.

[9]  Lester F. Eastman,et al.  Slow transients observed in AlGaN/GaN HFETs: effects of SiN/sub x/ passivation and UV illumination , 2003 .

[10]  Hideki Hasegawa,et al.  Mechanisms of current collapse and gate leakage currents in AlGaN/GaN heterostructure field effect transistors , 2003 .

[11]  Michael S. Shur,et al.  Mechanism of the reverse gate leakage in AlGaN/GaN high electron mobility transistors , 2003 .

[12]  S. Kishimoto,et al.  Surface potential measurements of AlGaN∕GaN high-electron-mobility transistors by Kelvin probe force microscopy , 2004 .

[13]  T. Nakayama,et al.  Improved power performance for a recessed-gate AlGaN-GaN heterojunction FET with a field-modulating plate , 2004, IEEE Transactions on Microwave Theory and Techniques.

[14]  Hideki Hasegawa,et al.  Leakage mechanism in GaN and AlGaN Schottky interfaces , 2004 .

[15]  Michael J. Uren,et al.  Direct demonstration of the ‘virtual gate’ mechanism for current collapse in AlGaN/GaN HFETs , 2005 .

[16]  I. Omura,et al.  Influence of surface defect charge at AlGaN-GaN-HEMT upon Schottky gate leakage current and breakdown voltage , 2005, IEEE Transactions on Electron Devices.

[17]  M. Kurouchi,et al.  Kelvin probe force microscopy study of surface potential transients in cleaved AlGaN/GaN high electron mobility transistors , 2007 .

[18]  Yuji Ando,et al.  Observation of cross-sectional electric field for GaN-based field effect transistor with field-modulating plate , 2007 .