Cavity standing-wave and gain compression coefficient in semiconductor lasers

1994 ◽  
Vol 19 (9) ◽  
pp. 640 ◽  
Author(s):  
Antonio Mecozzi
1999 ◽  
Vol 20 (3) ◽  
Author(s):  
Yonglin Tang ◽  
Yang Lu ◽  
Jianguo Chen ◽  
Dayi Li

1996 ◽  
Vol 32 (6) ◽  
pp. 981-985 ◽  
Author(s):  
H.M. Salgado ◽  
J.C.S. Castro ◽  
J.J. O'Reilly

Author(s):  
O.L. Krivanek ◽  
J. TaftØ

It is well known that a standing electron wavefield can be set up in a crystal such that its intensity peaks at the atomic sites or between the sites or in the case of more complex crystal, at one or another type of a site. The effect is usually referred to as channelling but this term is not entirely appropriate; by analogy with the more established particle channelling, electrons would have to be described as channelling either through the channels or through the channel walls, depending on the diffraction conditions.


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