grating vector
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Author(s):  
Frans Snik ◽  
David Doelman ◽  
Steven Bos ◽  
Mireille Ouellet ◽  
Michael Escuti ◽  
...  
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Author(s):  
Anna Boehle ◽  
Matthew A. Kenworthy ◽  
Adrian M. Glauser ◽  
Sascha P. Quanz ◽  
Frans Snik ◽  
...  
Keyword(s):  

Plasmonics ◽  
2015 ◽  
Vol 10 (5) ◽  
pp. 1049-1056 ◽  
Author(s):  
Kuo Pin Chiu ◽  
Yun Chorng Chang ◽  
Chiau Yuan Lai ◽  
Shih Hsuan Chen ◽  
Tsung Jhe Wu ◽  
...  

2015 ◽  
Vol 3 (42) ◽  
pp. 11011-11016 ◽  
Author(s):  
Jaana Vapaavuori ◽  
Robin H. A. Ras ◽  
Matti Kaivola ◽  
C. Geraldine Bazuin ◽  
Arri Priimagi

We demonstrate complete all-optical erasure of high-modulation-depth azopolymer surface patterns at ambient conditions. Applying selective optical erasure and rewriting can be translated into complex surface patterns with spatially varying grating vector directions.


2013 ◽  
Vol 21 (16) ◽  
pp. 19097 ◽  
Author(s):  
Tuan Guo ◽  
Fu Liu ◽  
Fa Du ◽  
Zhaochuan Zhang ◽  
Chunjie Li ◽  
...  

2013 ◽  
Vol 38 (4) ◽  
pp. 531 ◽  
Author(s):  
Tuan Guo ◽  
Libin Shang ◽  
Fu Liu ◽  
Chuang Wu ◽  
Bai-Ou Guan ◽  
...  

2007 ◽  
Vol 15 (1) ◽  
Author(s):  
G. Zakharyan ◽  
A. Galstyan

AbstractThe coupled wave theory of Raman and Nath diffraction is extended to the case of thin anisotropic holographic media with grating vector parallel to the medium boundaries. Solutions for the wave amplitudes, diffraction efficiencies, and angular mismatch sensitivities are given in transmission geometries for the case of mixed dielectric and absorption modulations. For an apparent distinction, the results are given only for dielectric modulation. The main difference of the new results, with respect to the expressions valid for isotropic media, arises due to the walk-off between the wave-front and energy propagation directions. The difference is particularly important in materials with large birefringence, such as organic crystals, ordered polymers, and liquid crystalline cells.


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