Nondestructive and simple method of optical-waveguide loss measurement with optimisation of end-fire coupling

1992 ◽  
Vol 28 (17) ◽  
pp. 1612 ◽  
Author(s):  
M. Haruna ◽  
Y. Segawa ◽  
H. Nishihara
1988 ◽  
Vol 27 (13) ◽  
pp. 2636 ◽  
Author(s):  
Robert K. Hickernell ◽  
Donald R. Larson ◽  
Robert J. Phelan ◽  
Lee E. Larson

2007 ◽  
Vol 39 (3) ◽  
pp. 532-536 ◽  
Author(s):  
G. Pandraud ◽  
H.T.M. Pham ◽  
P.J. French ◽  
P.M. Sarro

1995 ◽  
Vol 20 (17) ◽  
pp. 1773 ◽  
Author(s):  
Simon Brülisauer ◽  
Daniel Fluck ◽  
Carlo Solcia ◽  
Tomas Pliska ◽  
Peter Günter

2008 ◽  
Vol 20 (16) ◽  
pp. 1423-1425 ◽  
Author(s):  
W. H. Guo ◽  
D. Byrne ◽  
Q. Y. Lu ◽  
J. F. Donegan

Author(s):  
Jie Lin ◽  
Andreas Leven ◽  
R. Reyes ◽  
Y. K. Chen ◽  
Fow-sen Choa

2010 ◽  
Vol 3 (12) ◽  
pp. 122104 ◽  
Author(s):  
Dmitry S. Sizov ◽  
Rajaram Bhat ◽  
Albert Heberle ◽  
Kechang Song ◽  
Chung-en Zah

2011 ◽  
Vol 143-144 ◽  
pp. 644-648
Author(s):  
De En ◽  
Jie Yu Feng ◽  
Ning Bo Zhang ◽  
Ning Ning Wang ◽  
Xiao Bin Wang

The optical waveguides are produced in LiNbO3 substrate of three-component acceleration seismic geophone by lithography. Three-component acceleration seismic geophone detects changes in the external acceleration by detecting phase changes in the optical waveguides. The performance of optical waveguide directly affects the performance of three-component acceleration seismic geophone. Therefore, it is critical to measure and reduce the transmission loss of waveguides. The advantages and disadvantages of LiNbO3 crystal are introduced. The production process of Ti:LiNbO3 optical waveguide and its performance are presented. Some information about the types of transmission loss of optical waveguide and the measurement methods of optical waveguide loss are provided.


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