Transient transition of high speed and high- frequency ethanol droplet train impingement on the heated indium tin oxide (ITO) surface

Author(s):  
Baris Burak Kanbur ◽  
Marcus Lee Zhao Hui ◽  
Fei Duan
1995 ◽  
Author(s):  
Christian Beaulieu ◽  
Francois L. Gouin ◽  
Julian P. Noad ◽  
William Hartman ◽  
Ewa Lisicka-Skrzek ◽  
...  

2014 ◽  
Vol 21 (5) ◽  
pp. 732-735 ◽  
Author(s):  
Pi-Ying Cheng ◽  
Wen-Tse Hsiao ◽  
Chien-Kai Chung ◽  
Shih-Feng Tseng ◽  
Ien-Chang Liao

2001 ◽  
Vol 79 (17) ◽  
pp. 2838-2840 ◽  
Author(s):  
Necmi Biyikli ◽  
Tolga Kartaloglu ◽  
Orhan Aytur ◽  
Ibrahim Kimukin ◽  
Ekmel Ozbay

1994 ◽  
Vol 33 (Part 1, No. 7B) ◽  
pp. 4438-4441 ◽  
Author(s):  
Keiji Nakamura ◽  
Tomonori Imura ◽  
Hideo Sugai ◽  
Michiko Ohkubo ◽  
Katsutaro Ichihara

2003 ◽  
Vol 82 (14) ◽  
pp. 2344-2346 ◽  
Author(s):  
Necmi Biyikli ◽  
Ibrahim Kimukin ◽  
Tolga Kartaloglu ◽  
Orhan Aytur ◽  
Ekmel Ozbay

2011 ◽  
Vol 19 (2) ◽  
Author(s):  
P. Perkowski

AbstractIndium tin oxide (ITO) electrodes are widely used for liquid crystal applications as well as for measuring cells. Unfortunately, ITO layer possesses its own non zero resistivity R which produces (with the capacity C) the cut-off frequency f0 of RC circuit. Dielectric spectroscopy cannot be performed for high frequencies because of high frequency losses caused by the cell behaviour. Four procedures for estimating and extracting high frequency losses in ITO cells are presented and compared in this paper. Their limitations and viability are discussed.


2003 ◽  
Vol 764 ◽  
Author(s):  
Ibrahim Kimukin ◽  
Necmi Biyikli ◽  
Tolga Kartaloglu ◽  
Orhan Aytür ◽  
Ekmel Ozbay

AbstractWe have designed, fabricated and tested resonant cavity enhanced visible-blind AlGaN-based Schottky photodiodes. The bottom mirror of the resonant cavity was formed with a 20 pair AlN/AlGaN Bragg mirror. The devices were fabricated using a microwave compatible fabrication process. Au and indium-tin-oxide (ITO) thin films were used for Schottky contact formation. ITO and Au-Schottky devices exhibited resonant peaks with 0.153 A/W and 0.046 A/W responsivity values at 337 nm and 350 nm respectively. Temporal high-speed measurements at 357 nm resulted in fast pulse responses with pulse widths as short as 77 ps. The fastest UV detector had a 3-dB bandwidth of 780 MHz.


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