Theoretical and experimental study of the quasistatic capacitance of metal-insulator–hydrogenated amorphous silicon structures: Strong evidence for the defect-pool model

1998 ◽  
Vol 58 (16) ◽  
pp. 10401-10414 ◽  
Author(s):  
J. P. Kleider ◽  
F. Dayoub
1987 ◽  
Vol 95 ◽  
Author(s):  
G. Winborne ◽  
L. XU ◽  
M. Silver ◽  
H. M. Branz

AbstractExperimental results on the temporal response of i/n/i hydrogenated amorphous silicon structures are presented as a function of voltage. The current is initially space charge limited followed by a transition to an emission limited current. The data generally exhibits four subsequent time dependence regimes e.g. :(1) an exponential decay, (2) followed by a t−2 decay, (3) then a t−1 decay and (4) lastly a t(α−1) decay where α<1. The current versus time allows one to derive a density of states. The deduced density of states in the arsenic doped n layers displays a peak at shallow energies followed by an exponential with an energy decay constant of approximately 300°K followed by a flat region and finally followed by a slowly rising density of states. The initial Fermi level is estimated to be within the peak located less than 0.3eV from the mobility edge.


1994 ◽  
Vol 303 (1-2) ◽  
pp. 266-276 ◽  
Author(s):  
C.P. Lund ◽  
B.W. Clare ◽  
P.J. Jennings ◽  
J.C.L. Cornish ◽  
G.T. Hefter

1991 ◽  
Vol 219 ◽  
Author(s):  
J. Kanicki ◽  
C. Godet ◽  
A. V. Gelatos

ABSTRACTThe effects of positive and negative bias stress on hydrogenated amorphous silicon nitride / crystalline silicon and hydrogenated amorphous silicon nitride / hydrogenated amorphous silicon (a-Si:H) structures are investigated as a function of stress time, stress temperature and stress bias. It is shown that in both structures bias stress induces a parallel shift of the C-V (capacitance-voltage) characteristics. For a given stress bias the direction of the C-V shift depends on the sign of the applied stress voltage, while the magnitude of the C-V shift depends on stress time and temperature. In addition, it is shown that positive bias stress slightly increases the number of localized states in the a-Si:H mobility gap, but negative bias stress does not. These results lead us to conclude that the C-V shift is not induced by dangling bond defects in a-Si:H but rather by carrier trapping in the insulator.


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