Implementation of full-adder and full-subtractor based on electro-optic effect in Mach–Zehnder interferometers

2014 ◽  
Vol 324 ◽  
pp. 93-107 ◽  
Author(s):  
Ajay Kumar ◽  
Santosh Kumar ◽  
Sanjeev Kumar Raghuwanshi
Keyword(s):  
Author(s):  
Zhoufeng Ying ◽  
Zheng Wang ◽  
Shounak Dhar ◽  
Zheng Zhao ◽  
David Z. Pan ◽  
...  

2020 ◽  
Vol 52 (5) ◽  
Author(s):  
Foo Kui Law ◽  
M. Rakib Uddin ◽  
Chen Chen Teo ◽  
Bikash Nakarmi
Keyword(s):  

Author(s):  
Zhoufeng Ying ◽  
Zheng Wang ◽  
Shounak Dhar ◽  
Zheng Zhao ◽  
David Z. Pan ◽  
...  

Author(s):  
S. G. Ghonge ◽  
E. Goo ◽  
R. Ramesh ◽  
R. Haakenaasen ◽  
D. K. Fork

Microstructure of epitaxial ferroelectric/conductive oxide heterostructures on LaAIO3(LAO) and Si substrates have been studied by conventional and high resolution transmission electron microscopy. The epitaxial films have a wide range of potential applications in areas such as non-volatile memory devices, electro-optic devices and pyroelectric detectors. For applications such as electro-optic devices the films must be single crystal and for applications such as nonvolatile memory devices and pyroelectric devices single crystal films will enhance the performance of the devices. The ferroelectric films studied are Pb(Zr0.2Ti0.8)O3(PLZT), PbTiO3(PT), BiTiO3(BT) and Pb0.9La0.1(Zr0.2Ti0.8)0.975O3(PLZT).Electrical contact to ferroelectric films is commonly made with metals such as Pt. Metals generally have a large difference in work function compared to the work function of the ferroelectric oxides. This results in a Schottky barrier at the interface and the interfacial space charge is believed to responsible for domain pinning and degradation in the ferroelectric properties resulting in phenomenon such as fatigue.


1997 ◽  
Vol 7 (9) ◽  
pp. 1893-1898 ◽  
Author(s):  
G. Schirripa Spagnolo ◽  
D. Ambrosini ◽  
A. Ponticiello ◽  
D. Paoletti

2012 ◽  
Vol 132 (9) ◽  
pp. 727-733
Author(s):  
Masahiko Tani ◽  
Michael I. Bakunov ◽  
Kohji Yamamoto ◽  
Kazuki Horita ◽  
Tetsuya Kinoshita ◽  
...  

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