Very High Parallel-Plane Surface Electric Field of 4.3 MV/cm in Ga2O3 Schottky Barrier Diodes with PtOx Contacts

Author(s):  
Devansh Saraswat ◽  
Wenshen Li ◽  
Kazuki Nomoto ◽  
Debdeep Jena ◽  
Huili Grace Xing
2018 ◽  
Vol 4 (9) ◽  
pp. eaat9722 ◽  
Author(s):  
E Laine Wong ◽  
Andrew J. Winchester ◽  
Vivek Pareek ◽  
Julien Madéo ◽  
Michael K. L. Man ◽  
...  

2021 ◽  
Author(s):  
Peng Gao ◽  
Zhong-Hua Xue ◽  
Shi-Nan Zhang ◽  
Dong Xu ◽  
Guang-Yao Zhai ◽  
...  

2020 ◽  
Vol 116 (19) ◽  
pp. 192101 ◽  
Author(s):  
Wenshen Li ◽  
Devansh Saraswat ◽  
Yaoyao Long ◽  
Kazuki Nomoto ◽  
Debdeep Jena ◽  
...  

2013 ◽  
Vol 22 (10) ◽  
pp. 106107 ◽  
Author(s):  
Cen Tang ◽  
Gang Xie ◽  
Li Zhang ◽  
Qing Guo ◽  
Tao Wang ◽  
...  

2016 ◽  
Vol 136 (4) ◽  
pp. 479-483
Author(s):  
Masataka Higashiwaki ◽  
Kohei Sasaki ◽  
Hisashi Murakami ◽  
Yoshinao Kumagai ◽  
Akito Kuramata

1997 ◽  
Vol 473 ◽  
Author(s):  
Heng-Chih Lin ◽  
Edwin C. Kan ◽  
Toshiaki Yamanaka ◽  
Simon J. Fang ◽  
Kwame N. Eason ◽  
...  

ABSTRACTFor future CMOS GSI technology, Si/SiO2 interface micro-roughness becomes a non-negligible problem. Interface roughness causes fluctuations of the surface normal electric field, which, in turn, change the gate oxide Fowler-Nordheim tunneling behavior. In this research, we used a simple two-spheres model and a three-dimensional Laplace solver to simulate the electric field and the tunneling current in the oxide region. Our results show that both quantities are strong functions of roughness spatial wavelength, associated amplitude, and oxide thickness. We found that RMS roughness itself cannot fully characterize surface roughness and that roughness has a larger effect for thicker oxide in terms of surface electric field and tunneling behavior.


2020 ◽  
Vol 13 (9) ◽  
pp. 096502
Author(s):  
Yu Lu ◽  
Feng Zhou ◽  
Weizong Xu ◽  
Dongsheng Wang ◽  
Yuanyang Xia ◽  
...  

2019 ◽  
Vol 780 ◽  
pp. 476-481 ◽  
Author(s):  
Hong Gu ◽  
Cong Hu ◽  
Jiale Wang ◽  
Youming Lu ◽  
Jin-Ping Ao ◽  
...  

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