Surface photovoltage measurements and Fermi level pinning: comments on “development and confirmation of the unified model for Schottky barrier formation and MOS interface states on III-V compounds”

1982 ◽  
Vol 89 (4) ◽  
pp. L27-L33 ◽  
Author(s):  
L.J. Brillson
1992 ◽  
Vol 281 ◽  
Author(s):  
A. D. Marwick ◽  
M. O. Aboelfotoh ◽  
R. Casparis

ABSTRACTIt is shown that the presence of 8 × 1015 hydrogen atoms/cm2 in the CoSi2/Si (100) interface causes an increase in the Schottky barrier height of 120 meV, and that passivation of dopants in the substrate is not the cause of this change. The data is evidence that the position of the Fermi level in this interface is controlled by defect-related interface states. After hydrogenation the Schottky barrier height agrees with that predicted by theory for Fermi level pinning by virtual gap states of the silicon.


1982 ◽  
Vol 89 (4) ◽  
pp. 447-460 ◽  
Author(s):  
W.E. Spicer ◽  
S. Eglash ◽  
I. Lindau ◽  
C.Y. Su ◽  
P.R. Skeath

1987 ◽  
Vol 36 (3) ◽  
pp. 1647-1656 ◽  
Author(s):  
Jeffrey R. Lince ◽  
David J. Carré ◽  
Paul D. Fleischauer

2019 ◽  
Vol 9 (23) ◽  
pp. 5014
Author(s):  
Courtin ◽  
Moréac ◽  
Delhaye ◽  
Lépine ◽  
Tricot ◽  
...  

Fermi level pinning at metal/semiconductor interfaces forbids a total control over the Schottky barrier height. 2D materials may be an interesting route to circumvent this problem. As they weakly interact with their substrate through Van der Waals forces, deposition of 2D materials avoids the formation of the large density of state at the semiconductor interface often responsible for Fermi level pinning. Here, we demonstrate the possibility to alleviate Fermi-level pinning and reduce the Schottky barrier height by the association of surface passivation of germanium with the deposition of 2D graphene.


1999 ◽  
Vol 86 (12) ◽  
pp. 6890-6894 ◽  
Author(s):  
M. Mamor ◽  
O. Nur ◽  
M. Karlsteen ◽  
M. Willander ◽  
F. D. Auret

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