Application of nano-pulsed Nd:YAG laser to crystallization of amorphous Si thin films for next generation flat-panel display

Author(s):  
Jaewon Lee ◽  
Jin-Ha Hwang ◽  
Sang Won Lee ◽  
Seungho Park ◽  
Seungwon Shin ◽  
...  
2002 ◽  
Vol 49 (1) ◽  
pp. 221-229 ◽  
Author(s):  
W. Zhu ◽  
O. K. Tan ◽  
J. Ray ◽  
Md A. Imam ◽  
X. F. Chen

2007 ◽  
Vol 32 (2) ◽  
pp. 497-500 ◽  
Author(s):  
Daisuke Tsukiyama ◽  
Kousuke Takenaka ◽  
Yuichi Setsuhara ◽  
Kazuaki Nishisaka ◽  
Akinori Ebe

2001 ◽  
Vol 40 (Part 1, No. 2B) ◽  
pp. 1061-1063 ◽  
Author(s):  
Yoshiaki Suda ◽  
Kazuya Doi ◽  
Jun Namba ◽  
Fumiaki Imura ◽  
Hiroharu Kawasaki

2009 ◽  
Vol 517 (14) ◽  
pp. 4061-4064 ◽  
Author(s):  
Se Il Kim ◽  
Sang Hyun Cho ◽  
Sung Ryong Choi ◽  
Min Cheol Oh ◽  
Ji Hyang Jang ◽  
...  

2017 ◽  
Author(s):  
Hsing-Chieh Lee ◽  
Ying-Hao Lu ◽  
Shin-Yih Huang ◽  
Wei-Jen Lan ◽  
Makoto Hanabata

Author(s):  
Reo Usui ◽  
Ryohei Satoh ◽  
Yoshiharu Iwata ◽  
Koji Nakagawa ◽  
Eiji Morinaga ◽  
...  

2000 ◽  
Vol 617 ◽  
Author(s):  
Hiroharu Kawasaki ◽  
Kazuya Doi. Jun Namba ◽  
Yoshiaki Suda

AbstractTantalum nitride (TAN) films have been deposited on silicon substrates by using a pulsed Nd:YAG laser deposition method. Experimental results suggest that the substrate temperature is one of the most important parameters to prepare crystalline tantalum nitride thin films. Glancing-angle X-ray diffraction patterns show that the films deposited at Ts ≤ 300 °C are almost amorphous. and crystalline Ta6N2.57 films are obtained at Ts ≥ 500 °C. Grain size of the film increases with increasing substrate temperature.


2000 ◽  
Vol 617 ◽  
Author(s):  
Kazuya Doi ◽  
Satoshi Hiraishi ◽  
Hiroharu Kawasaki ◽  
Yoshiaki Suda

AbstractChromium carbide thin films are synthesized on Si(100) substrates by a pulsed Nd:YAG laser deposition (PLD) method as parameters of methane gas pressure. Glancing-angle X-ray diffraction patterns show that the film prepared by PLD method is a polycrystalline thin film composed of Cr3C2and Cr7C3, even in the base pressure. Diffraction patterns, however, are depended on the methane gas pressure. Grain size of the prepared film increases with increasing methane gas pressure. One of the reasons of these phenomena may be considered to the phase reaction between the ablated species, such as Cr, CrCx and CH4gas in the plasma plume.


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