Role of Cation Dissociation in Schottky Barrier Formation at II–VI Compound Semiconductor-Metal Interfaces

1981 ◽  
Vol 10 ◽  
Author(s):  
C. F. Brucker ◽  
L. J. Brillson

We used UV and X-ray photoemission spectroscopies to probe the relation between the chemical and electronic structure at ultrahigh-vacuum-cleaved CdS-metal and CdSe-metal interfaces. When combined with current-voltage and capacitance-voltage studies of the same interfaces in ultrahigh vacuum, the experimental results indicate that partially dissociated cadmium cations, produced as a consequence of interfacial chemical reaction, may be the electrically active species giving rise to the observed Fermi level stabilization at these contacts. The extent of cation dissociation, a spectroscopically determined quantity, is shown to correlate inversely with the measured Schottky barrier height. An indirect and modified doping effect is suggested as one possible mechanism to explain this behavior. Features of interdiffusion, in particular regarding the interfacial distribution of dissociated cadmium, are also described.

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.


Author(s):  
H. L. Mosbacker ◽  
S. El Hage ◽  
M. Gonzalez ◽  
S. A. Ringel ◽  
M. Hetzer ◽  
...  

2013 ◽  
Vol 43 (1-2) ◽  
pp. 13-21 ◽  
Author(s):  
Y. Munikrishana Reddy ◽  
M. K. Nagaraj ◽  
M. Siva Pratap Reddy ◽  
Jung-Hee Lee ◽  
V. Rajagopal Reddy

1995 ◽  
Vol 395 ◽  
Author(s):  
A.C. Schmitz ◽  
A.T. Ping ◽  
M. Asif khan ◽  
I. Adesida

ABSTRACTSchottky barrier heights of Ni, Pt, Pd, and Au on n-type GaN were measured using current-voltage and capacitance-voltage techniques. Measurements from the I-V technique yielded barrier heights of 0.95, 1.01, 0.94, and 0.87 eV for Ni, Pt, Pd, and Au, respectively. Barrier heights of 1.13,1.16, 1.07, and 0.98 eV, for Ni, Pt, Pd, and Au, respectively, were obtained using C-V measurements.


Silicon ◽  
2018 ◽  
Vol 11 (6) ◽  
pp. 2647-2657 ◽  
Author(s):  
Durmuş Ali Aldemir ◽  
Rukiye Aldemir ◽  
Ali Kökce ◽  
Songül Duman ◽  
Ahmet Faruk Özdemir

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