EFFECTS OF BUFFER LAYER THICKNESS AND DOPING CONCENTRATION ON SiC MESFET CHARACTERISTICS

Author(s):  
SANKHA S. MUKHERJEE ◽  
SYED S. ISLAM
2004 ◽  
Vol 14 (03) ◽  
pp. 890-896 ◽  
Author(s):  
SANKHA S. MUKHERJEE ◽  
SYED S. ISLAM

Two-dimensional simulations have been carried out using the Atlas® device simulator to investigate the effects of the buffer layer thickness and doping concentration on the electrical characteristics of the SiC MESFET. The variations of transconductance, output resistance, gate-source capacitance, gate-drain capacitance and (cutoff frequency) f T with respect to the change in buffer layer thickness and doping concentration have been investigated. It is observed that the performances of MESFET can be improved by reducing the leakage of channel carrier into the substrate at high drain bias, which is achieved by increasing buffer layer doping density and/or increasing buffer layer thickness. For a SiC MESFET with buffer layer thickness of 0.3μm and gate length of 1μm, drain current increases from 0.1A/ μm to above 0.45A/ μm as the buffer layer doping density is decreased from 1.9 × 1017 cm -3 to 1 × 1016 cm -3. The simulations were carried out at a gate-source voltage of –1V and a drain-source voltage of 15V. Under similar conditions, the output resistance decreases from 1.2 × 106 Ω/μ m to 1.2 × 106 Ω/μ m , and the transconductance decreases from 5.9mS/ μm to 5.3mS/ μm, and f T decreases from 11GHz to 8GHz.


2011 ◽  
Vol 11 (2) ◽  
pp. 1409-1412 ◽  
Author(s):  
Ah Ra Kim ◽  
Ju-Young Lee ◽  
Bo Ra Jang ◽  
Hong Seung Kim ◽  
Young Ji Cho ◽  
...  

2010 ◽  
Vol 19 (3) ◽  
pp. 036801 ◽  
Author(s):  
Wu Yu-Xin ◽  
Zhu Jian-Jun ◽  
Chen Gui-Feng ◽  
Zhang Shu-Ming ◽  
Jiang De-Sheng ◽  
...  

1994 ◽  
Vol 339 ◽  
Author(s):  
T. J. Kistenmacher ◽  
S. A. Ecelberger ◽  
W. A. Bryden

ABSTRACTIntroduction of a buffer layer to facilitate heteroepitaxy in thin films of the Group IIIA nitrides has had a tremendous impact on growth morphology and electrical transport. While AIN- and self-seeded growth of GaN has captured the majority of attention, the use of AIN-buffered substrates for InN thin films has also had considerable success. Herein, the properties of InN thin films grown by reactive magnetron sputtering on AIN-buffered (00.1) sapphire and (111) silicon are presented and, in particular, the evolution of the structural and electrical transport properties as a function of buffer layer sputter time (corresponding to thicknesses from ∼50Å to ∼0.64 μm) described. Pertinent results include: (a) for the InN overlayer, structural coherence and homogeneous strain normal to the (00.1) growth plane are highly dependent on the thickness of the AIN-buffer layer; (b) the homogeneous strain in the AIN-buffer layer is virtually nonexistent from a thickness of 200Å (where a significant X-ray intensity for (00.2)AIN is observed); and (c) the n-type electrical mobility for films on AIN-nucleated (00.1) sapphire is independent of AIN-buffer layer thickness, owing to divergent variations in carrier concentration and film resistivity. These effects are in the main interpreted as arising from a competition between the lattice mismatch of the InN overlayer with the substrate and with the AIN-buffer layer.


2004 ◽  
Vol 262 (1-4) ◽  
pp. 456-460 ◽  
Author(s):  
Yuantao Zhang ◽  
Guotong Du ◽  
Boyang Liu ◽  
HuiChao Zhu ◽  
Tianpeng Yang ◽  
...  

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