Experimental Analysis of the Schottky Barrier Layer Model for Reduced Rutile Diodes

1964 ◽  
Vol 35 (7) ◽  
pp. 2142-2144 ◽  
Author(s):  
Richard Bechtel
1998 ◽  
Vol 45 (7) ◽  
pp. 1595-1604 ◽  
Author(s):  
K.P. Schoen ◽  
J.M. Woodall ◽  
J.A. Cooper ◽  
M.R. Melloch

2016 ◽  
Vol 213 (4) ◽  
pp. 889-892 ◽  
Author(s):  
Ji Hyun Hwang ◽  
Se-Mi Kim ◽  
Jeong Min Woo ◽  
Sung-Min Hong ◽  
Jae-Hyung Jang

2019 ◽  
Vol 73 ◽  
pp. 24-47 ◽  
Author(s):  
A. Lucarelli ◽  
C. Lugni ◽  
M. Falchi ◽  
M. Felli ◽  
M. Brocchini

Assuming an arbitrary distribution of space charge in the barrier layer of a rectifier, the general form of the current-voltage relation has been derived on both diode and diffusion theory. A connexion, valid for most barriers, between this characteristic and the capacitance-voltage curve has been pointed out, and it has been shown that the Sachs breakdown voltage can be deduced from the latter characteristic. The general relations have been applied to a barrier whose distribution of impurity centres is assumed to establish itself by a diffusion process. Its properties have been investigated, and it has been found that the shapes of the experimental d. c. characteristics, considered in a previous paper (Landsberg 1951 b ), are in the same good agreement with the hypothesis of this barrier as they are with the hypothesis of a Schottky barrier. The difficulties regarding the constants of the rectifiers , as obtained from the experimental curves, are, however, greatly alleviated if the present barriers rather than Schottky’s barrier is assumed. It has been shown that both barriers belong to a whole class of barrier layers whose d. c. and capacitance-voltage curves have the same shape as the corresponding curves for a Schottky barrier.


2016 ◽  
Author(s):  
J.W. Chiu ◽  
S.C. Chen ◽  
B.H. Li ◽  
H.C. Chiu ◽  
R. Xuan ◽  
...  

2000 ◽  
Vol 166 (1-4) ◽  
pp. 485-491 ◽  
Author(s):  
Hiro Niimi ◽  
Hanyang Yang ◽  
Gerald Lucovsky ◽  
Jeff W Keister ◽  
Jack E Rowe

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