Fast optical inspection of operations of large-area active-matrix backplane by gate modulation imaging

2018 ◽  
Vol 55 ◽  
pp. 187-193 ◽  
Author(s):  
Jun'ya Tsutsumi ◽  
Satoshi Matsuoka ◽  
Toshihide Kamata ◽  
Tatsuo Hasegawa
ACS Nano ◽  
2019 ◽  
Vol 13 (3) ◽  
pp. 3023-3030 ◽  
Author(s):  
Yong Ju Park ◽  
Bhupendra K. Sharma ◽  
Sachin M. Shinde ◽  
Min-Seok Kim ◽  
Bongkyun Jang ◽  
...  

Author(s):  
Jan-Laurens P.J. van der Steen ◽  
Laurens C.J.M. Peters ◽  
Edsger C.P. Smits ◽  
Peter Zalar ◽  
Gerwin H. Gelinck

2010 ◽  
Vol 57 (5) ◽  
pp. 995-1002 ◽  
Author(s):  
Yusaku Kato ◽  
Tsuyoshi Sekitani ◽  
Yoshiaki Noguchi ◽  
Tomoyuki Yokota ◽  
Makoto Takamiya ◽  
...  

2009 ◽  
Vol 1153 ◽  
Author(s):  
Ruud E.I. Schropp ◽  
Zomer Silvester Houweling ◽  
Vasco Verlaan

AbstractHot Wire Chemical Vapor Deposition (HWCVD) is a fast deposition technique with high potential for homogeneous deposition of thin films on large area panels or on continuously moving substrates in an in-line manufacturing system. As there are no high-frequency electromagnetic fields, scaling up is not hampered by finite wavelength effects or the requirement to avoid inhomogeneous electrical fields. Since 1996 we have been investigating the application of the HWCVD process for thin film transistor manufacturing. It already appeared then that these Thin Film Transistors (TFTs) were electronically far more stable than those with Plasma Enhanced (PE) CVD amorphous silicon. Recently, we demonstrated that very compact SiNx layers can be deposited at high deposition rates, up to 7 nm/s. The utilization of source gases in HWCVD of a-Si3N4 films deposited at 3 nm/s is 75 % and 7 % for SiH4 and NH3, respectively. Thin films of stoichiometric a-Si3N4 deposited at this rate have a high mass-density of 3.0 g/cm3. The dielectric properties have been evaluated further in order to establish their suitability for incorporation in TFTs. Now that all TFT layers, namely, the SiNx insulator, the a-Si:H or μc Si:H layers, and the n-type doped thin film silicon can easily be manufactured by HWCVD, the prospect of “all HWCVD” TFTs for active matrix production is within reach. We tested the 3 nm/s SiNx material combined with our protocrystalline Si:H layers deposited at 1 nm/s in ‘all HW’ TFTs. Results show that the TFTs are state of the art with a field-effect mobility of 0.4 cm2/Vs. In order to assess the feasibility of large area deposition we are investigating in-line HWCVD for displays and solar cells.


1992 ◽  
Vol 19 (1-4) ◽  
pp. 187-190 ◽  
Author(s):  
J. Farrell ◽  
M. Westcott ◽  
A. Van Calster ◽  
J. De Baets ◽  
I. De Rycke ◽  
...  

1986 ◽  
Vol 33 (8) ◽  
pp. 1212-1217 ◽  
Author(s):  
T. Sunata ◽  
T. Yukawa ◽  
K. Miyake ◽  
Y. Matsushita ◽  
Y. Murakami ◽  
...  

2007 ◽  
Vol 989 ◽  
Author(s):  
Nader Safavian ◽  
Y. Vygranenko ◽  
J. Chang ◽  
Kyung Ho Kim ◽  
J. Lai ◽  
...  

AbstractBecause of the inherent desired material and technological attributes such as low temperature deposition and high uniformity over large area, the amorphous silicon (a-Si:H) technology has been extended to digital X-ray diagnostic imaging applications. This paper reports on design, fabrication, and characterization of a MIS-type photosensor that is fully process-compatible with the active matrix a-Si:H TFT backplane. We discuss the device operating principles, along with measurement results of the transient dark current, linearity and spectral response.


2004 ◽  
Vol 35 (1) ◽  
pp. 1284 ◽  
Author(s):  
N. C. van der Vaart ◽  
H. Lifka ◽  
F. P. M. Budzelaar ◽  
J. E. J. M. Rubingh ◽  
J. J. L. Hoppenbrouwers ◽  
...  
Keyword(s):  

1993 ◽  
Vol 297 ◽  
Author(s):  
C Van Berkel ◽  
N C Bird ◽  
C J Curling ◽  
I D French

2D image sensor arrays made with a-Si devices on glass over large area are of considerable interest as document scanners and in medical applications. We have made a test array containing a-Si NIP diodes for both the sensors and the active matrix switching devices. The issues of vertical crosstalk and image lag are discussed in relation to the device performance of the switching diode. The vertical crosstalk is controlled by the diode capacitance and the image lag by the high transient current in the device. We speculate that the transient current is a trap filling current in the deep states of the switching diode.


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