Magneto‐optic nonreciprocal phase shift in (YLa)3(FeGa)5O12single‐mode channel waveguides

1988 ◽  
Vol 64 (3) ◽  
pp. 1575-1577 ◽  
Author(s):  
H. Inuzuka ◽  
Y. Okamura ◽  
S. Yamamoto
1993 ◽  
Vol 74 (8) ◽  
pp. 4877-4881 ◽  
Author(s):  
Toshihiro Shintaku ◽  
Takehiko Uno ◽  
Morio Kobayashi

Optik ◽  
2019 ◽  
Vol 179 ◽  
pp. 641-645
Author(s):  
Cui Liang ◽  
Dengwei Zhang ◽  
Xiaowu Shu ◽  
Cheng Liu

1999 ◽  
Vol 74 (20) ◽  
pp. 2918-2920 ◽  
Author(s):  
M. Fehndrich ◽  
A. Josef ◽  
L. Wilkens ◽  
J. Kleine–Börger ◽  
N. Bahlmann ◽  
...  

1995 ◽  
Vol 20 (16) ◽  
pp. 1740 ◽  
Author(s):  
R. Wolfe ◽  
W.-K. Wang ◽  
D. J. DiGiovanni ◽  
A. M. Vengsarkar
Keyword(s):  

2011 ◽  
Vol 1291 ◽  
Author(s):  
Tetsuya Mizumoto ◽  
Ryohei Takei

ABSTRACTSurface activated direct bonding of a magnetooptic garnet crystal to a Silicon-On-Insulator (SOI) wafer is discussed for the application to waveguide optical nonreciprocal devices. An interferometric waveguide isolator is discussed that uses nonreciprocal phase shift brought about by a first-order magneto-optic effect. In an SOI waveguide, the low refractive index of buried oxide layer enhances the magneto-optic phase shift. This contributes to reduce the device size together with the strong field confinement of high index contrast waveguide. The interferometric isolator can be extended to an optical circulator by adopting appropriate 3-dB directional couplers to construct a Mach-Zehnder interferometer.


1990 ◽  
Author(s):  
Stefan Nowarra ◽  
Dietmar Seidenberg ◽  
Norbert Thorweihe ◽  
Hans J. Schmitt

1990 ◽  
Vol 68 (8) ◽  
pp. 3849-3855 ◽  
Author(s):  
E. Pross ◽  
H. Dammann ◽  
W. Tolksdorf

2008 ◽  
Vol 44 (2) ◽  
pp. 203-207 ◽  
Author(s):  
Gishamol Mathew ◽  
Anju Babu ◽  
Jesly Jacob ◽  
Vincent Mathew

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