Material Properties Controlling the Performance of Amorphous Silicon Thin Film Transistors

1984 ◽  
Vol 33 ◽  
Author(s):  
M. J. Powell

ABSTRACTAmorphous silicon thin film transistors have been fabricated with a number of different structures and materials. To date, the best performance is obtained with amorphous silicon - silicon nitride thin film transistors in the inverted staggered electrode structure, where the gate insulator and semiconductor are deposited sequentially by plasma enhanced chemical vapour deposition in the same growth apparatus.Localised electron states in the amorphous silicon are crucial in determining transistor performance. Conduction band states (Si-Si antibonding σ*) are broadened and localised in the amorphous network, and their energy distribution determines the field effect mobility. The silicon dangling bond defect is the most important deep localised state and their density determines the prethreshold current and hence the threshold voltage. The density of states is influenced by the gate insulator interface and there is probably a decreasing density of states away from this interface. The silicon dangling bond defect in the bulk amorphous silicon nitride also leads to a localised gap state, which is responsible for the observed threshold voltage instability.Other key material properties include the fixed charge densities associated with primary passivating layers placed on top of the amorphous silicon. The low value of the bulk density of states in the amorphous silicon layer increases the sensitivity of device characteristics to charge at the top interface.

2008 ◽  
Vol 22 (04) ◽  
pp. 263-268
Author(s):  
YONG K. LEE

The hydrogenerated amorphous silicon a-Si:H thin film transistors TFT with silicon nitride as a gate insulator have been stressed with independently varying gate (Vg), source (Vs), and gate-source (Vgs) bias voltage in order to elucidate the instability mechanism and suggest the new a-Si:H TFT structure. It was found that there was dependency of threshold voltage shift not only on Vgs, but also on Vg and Vs, which had not ever been reported. Its shift amount increased with increasing Vs and/or Vg. In this reports, we suggested the new TFT device structure to eliminate the dependency of Vth shift on Vg and Vs and found that with the new suggested TFT structure, the Vth shift controlling factor can only be Vgs.


1996 ◽  
Vol 424 ◽  
Author(s):  
Jeong Hyun Kim ◽  
Woong Sik Choi ◽  
Chan Hee Hong ◽  
Hoe Sup Soh

AbstractThe off current behavior of hydrogenated amorphous silicon (a-Si:H) thin film transistors (TFTs) with an atmospheric pressure chemical vapor deposition (APCVD) silicon dioxide (SiO2) gate insulator were investigated at negative gate voltages. The a-Si:H TFT with SiO2 gate insulator has small off currents and large activation energy (Ea) of the off current compared to the a-Si:H TFT with SiNx gate insulator. The holes induced in the channel by negative gate voltage seem to be trapped in the defect states near the a-Si:H/SiO2 interface. The interface state density in the lower half of the band gap of a-Si:H/SiO2 appears to be much higher than that for a-Si:H/SiNx.


1990 ◽  
Vol 192 ◽  
Author(s):  
Tetsu Ogawa ◽  
Sadayoshi Hotta ◽  
Horoyoshi Takezawa

ABSTRACTThrough the time and temperature dependence measurements on threshold voltage shifts (Δ VT) in amorphous silicon thin film transistors, it has been found that two separate instability mechanisms exist; within short stress time ranges Δ Vτ increases as log t and this behavior corresponds to charge trapping in SiN. On the other hand, in long stress time ranges Δ VT increases as t t/4 and can be explained by time-dependent creation of trap in a-Si.


1991 ◽  
Vol 30 (Part 1, No. 12B) ◽  
pp. 3719-3723 ◽  
Author(s):  
Ryoji Oritsuki ◽  
Toshikazu Horii ◽  
Akira Sasano ◽  
Ken Tsutsui ◽  
Toshiko Koizumi ◽  
...  

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