Relationship between Mobilities from Time-of-Flight and Dark-Injection Space-Charge-Limited Current Measurements for Organic Semiconductors: A Monte Carlo Study

2014 ◽  
Vol 118 (12) ◽  
pp. 6052-6058 ◽  
Author(s):  
Haoyuan Li ◽  
Lian Duan ◽  
Deqiang Zhang ◽  
Guifang Dong ◽  
Juan Qiao ◽  
...  
2012 ◽  
Vol 13 (9) ◽  
pp. 1700-1709 ◽  
Author(s):  
P. López Varo ◽  
J.A. Jiménez Tejada ◽  
J.A. López Villanueva ◽  
J.E. Carceller ◽  
M.J. Deen

2013 ◽  
Vol 4 ◽  
pp. 180-188 ◽  
Author(s):  
Thomas Kirchartz

Numerical simulations of current–voltage curves in electron-only devices are used to discuss the influence of charged defects on the information derived from fitting space-charge-limited current models to the data. Charged, acceptor-like defects lead to barriers impeding the flow of electrons in electron-only devices and therefore lead to a reduced current that is similar to the situation where the device has a built-in voltage. This reduced current will lead to an underestimation of the mobilities and an overestimation of characteristic tail slopes if analytical equations are used to analyze the data. Correcting for the barrier created by the charged defects can, however, be a successful way to still be able to obtain reasonably accurate mobility values.


RSC Advances ◽  
2014 ◽  
Vol 4 (67) ◽  
pp. 35344 ◽  
Author(s):  
Kwang Hee Cheon ◽  
Jangwhan Cho ◽  
Byung Tack Lim ◽  
Hui-Jun Yun ◽  
Soon-Ki Kwon ◽  
...  

1966 ◽  
Vol 2 (7) ◽  
pp. 282
Author(s):  
A.M. Phahle ◽  
K.C. Kao ◽  
J.H. Calderwood

1995 ◽  
Vol 377 ◽  
Author(s):  
G. J. Adriaenssens ◽  
B. Yan ◽  
A. Eliat

ABSTRACTA full and detailed transient space-charge-limited current (T-SCLC) study of a-Si:H p-i-n diodes has been carried out in the time range from 108s to 10s. In the short-time regime, general features of T-SCLC such as the current cusp and the carrier extraction period were observed, and related transport parameters were deduced. Electron emission from deep states was studied by measuring the current transients well beyond the extraction time. The emission time is thermally activated at temperatures higher than 250K and levels off at lower temperatures. The high temperature behaviour places the upper edge of the deep states at 0.42–0.52eV below the conduction band edge, and the attempt-to-escape frequency in the range of 1011-1013Hz. An observed shift of emission time with light intensity is attributed to defect relaxation.


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