P‐1.14: The Influence of Bottom gate Dielectric Roughness on the Performance of Double‐Gate a‐IGZO Thin Film Transistors

2019 ◽  
Vol 50 (S1) ◽  
pp. 677-680
Author(s):  
Ludong Qin ◽  
Xuan Deng ◽  
Jinao Tao ◽  
Shengdong Zhang
2007 ◽  
Vol 124-126 ◽  
pp. 383-386
Author(s):  
Jae Bon Koo ◽  
Jung Wook Lim ◽  
Chan Hoe Ku ◽  
Sang Chul Lim ◽  
Jung Hun Lee ◽  
...  

We report on the fabrication of dual-gate pentacene organic thin-film transistors (OTFTs) using a plasma-enhanced atomic layer deposited (PEALD) 150 nm thick Al2O3 as a bottom gate dielectric and a 300 nm thick parylene or a PEALD 200 nm thick Al2O3 as both a top gate dielectric and a passivation layer. The threshold voltage (Vth) of OTFT with a 300 nm thick parylene as a top gate dielectric is changed from 4.7 V to 1.3 V and that with a PEALD 200 nm thick Al2O3 as a top gate dielectric is changed from 1.95 V to -9.8 V when the voltage bias of top gate electrode is changed from -10 V to 10 V. The change of Vth of OTFT with the dual-gate structure has been successfully understood by an analysis of electrostatic potential.


2020 ◽  
Vol 7 (10) ◽  
pp. 1902145 ◽  
Author(s):  
Michael Geiger ◽  
Rachana Acharya ◽  
Eric Reutter ◽  
Thomas Ferschke ◽  
Ute Zschieschang ◽  
...  

2007 ◽  
Vol 102 (6) ◽  
pp. 064512 ◽  
Author(s):  
Mohammad R. Esmaeili-Rad ◽  
Flora Li ◽  
Andrei Sazonov ◽  
Arokia Nathan

1999 ◽  
Vol 557 ◽  
Author(s):  
Eugene Ma ◽  
Sigurd Wagner

AbstractWe report a novel TFT structure where the gate metal is embedded into a SiNx passivation layer. This allows the subsequent gate dielectric layer to be much thinner than in conventional bottom-gate structures. thereby reducing the threshold voltage and the sub-threshold slope. TFTs employing these damascene-gate structures were fabricated with SiNX gate dielectrics as thin as 50 nm. Such devices exhibit threshold voltages of 0.9 V, sub-threshold slopes of 0.1 V/dec, ION/IOFF current ratios of 106 and linear region field-effect mobilities of 0.6 cm2/Vs.


1990 ◽  
Vol 182 ◽  
Author(s):  
T. Y. Huang ◽  
C. C. Tsai ◽  
I. W. Wu ◽  
A. G. Lewis ◽  
A. Chiang ◽  
...  

AbstractA new process architecture for fabricating CMOS thin film transistors (TFTs) using in-situ-doped polysilicon source-drain layers is proposed. In the new architecture, a top-gate n-channel TFT and a bottom-gate p-channel TFT, or vice versa, form a CMOS pair. This allows an n+ - doped polysilicon bottom (or top) layer to serve simultaneously as the source-drain layer of the n-channel TFTs and the gate layer of the p-channel TFTs; while a p+ - doped polysilicon top (or bottom) layer serves as the source-drain layer of the p-channel TFT and the gate layer of the n-channel TFT. It thus eliminates the deposition of a separate doped gate layer normally required in the conventional process flow. In addition, a thin tri-layer stack, consisting of undoped-poly / gate dielectric / undoped-poly, separates the two doped polysilicon layers, thus allowing the use of a single island mask to define the channel regions for both the n- and p-channel TFTs. As a result, the photolithographic steps are also reduced by one mask. Working n- and p-channel TFTs with both top- and bottomgate structures, obtained by reversing the dopant types of the top and the bottom layers, have been successfully demonstrated using low-temperature (< 600 °C) polysilicon technology.


Micromachines ◽  
2021 ◽  
Vol 12 (3) ◽  
pp. 327
Author(s):  
Je-Hyuk Kim ◽  
Jun Tae Jang ◽  
Jong-Ho Bae ◽  
Sung-Jin Choi ◽  
Dong Myong Kim ◽  
...  

In this study, we analyzed the threshold voltage shift characteristics of bottom-gate amorphous indium-gallium-zinc-oxide (IGZO) thin-film transistors (TFTs) under a wide range of positive stress voltages. We investigated four mechanisms: electron trapping at the gate insulator layer by a vertical electric field, electron trapping at the drain-side GI layer by hot-carrier injection, hole trapping at the source-side etch-stop layer by impact ionization, and donor-like state creation in the drain-side IGZO layer by a lateral electric field. To accurately analyze each mechanism, the local threshold voltages of the source and drain sides were measured by forward and reverse read-out. By using contour maps of the threshold voltage shift, we investigated which mechanism was dominant in various gate and drain stress voltage pairs. In addition, we investigated the effect of the oxygen content of the IGZO layer on the positive stress-induced threshold voltage shift. For oxygen-rich devices and oxygen-poor devices, the threshold voltage shift as well as the change in the density of states were analyzed.


1996 ◽  
Vol 424 ◽  
Author(s):  
R. E. I. Schropp ◽  
K. F. Feenstra ◽  
C. H. M. Van Der Werf ◽  
J. Holleman ◽  
H. Meiling

AbstractWe present the first thin film transistors (TFTs) incorporating a low hydrogen content (5 - 9 at.-%) amorphous silicon (a-Si:H) layer deposited by the Hot-Wire Chemical Vapor Deposition (HWCVD) technique. This demonstrates the possibility of utilizing this material in devices. The deposition rate by Hot-Wire CVD is an order of magnitude higher than by Plasma Enhanced CVD. The switching ratio for TFTs based on HWCVD a-Si:H is better than 5 orders of magnitude. The field-effect mobility as determined from the saturation regime of the transfer characteristics is still quite poor. The interface with the gate dielectric needs further optimization. Current crowding effects, however, could be completely eliminated by a H2 plasma treatment of the HW-deposited intrinsic layer. In contrast to the PECVD reference device, the HWCVD device appears to be almost unsensitive to bias voltage stressing. This shows that HW-deposited material might be an approach to much more stable devices.


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