Octupolar Molecules for Nonlinear Optics: From Molecular Design to Crystals and Films with Large Second-Harmonic Generation

2014 ◽  
Vol 15 (1) ◽  
pp. 132-142 ◽  
Author(s):  
Mi-Yun Jeong ◽  
Bong Rae Cho
1989 ◽  
Vol 175 ◽  
Author(s):  
T. Ishii ◽  
T. Wada ◽  
A. F. Garito ◽  
H. Sasabe ◽  
A. Yamada

AbstractSecond order molecular susceptibilities β of poly(γ – benzyl L–glutamate)(PBLG) and poly(γ – p–nitrobenzyl L–glutamate) (PNBLG) were determined by means of dc-induced second harmonic generation (dc-SHG technique in solutions at a wavelength of 1064nm as 1.5×10–−29 esu and −4.9×10−29 esu, respectively. Among PBLG, PNBLG and nitrobenzene, it was found that only PNBLG has negative value of β. It follows that the effect of nitrophenyl groups in side chains is dominant for β whereas the contribution of carbonyl groups in main chain is dominant for the permanent dipole moment μ in PNBLG.


1995 ◽  
Vol 413 ◽  
Author(s):  
G. I. Stegeman ◽  
M. JÄger ◽  
A. Otomo ◽  
W. Brinker ◽  
S. Yilmaz ◽  
...  

ABSTRACTThe phenomenon of second harmonic generation has been studied from the earliest days of nonlinear optics.[l] To date the most impressive results in terms of conversion efficiency for as low an input power as possible have been obtained in channel waveguides made from inorganic materials.[2] However, when their second order nonlinearities (10s of pm/V) are compared with those of organic materials (10s → 100s pmn/V), it is clear that organic materials should eventually produce much better harmonic conversion efficiencies. [3]


2006 ◽  
Author(s):  
Dominique Chauvat ◽  
Loc Le Xuan ◽  
François Marquier ◽  
Sophie Brasselet ◽  
François Treussart ◽  
...  

2018 ◽  
Vol 28 (51) ◽  
pp. 1870367
Author(s):  
Yuan Zeng ◽  
Haoliang Qian ◽  
Matthew J. Rozin ◽  
Zhaowei Liu ◽  
Andrea R. Tao

2019 ◽  
Vol 100 (5) ◽  
Author(s):  
Hai-Jun Wu ◽  
Hao-Ran Yang ◽  
Carmelo Rosales-Guzmán ◽  
Wei Gao ◽  
Bao-Sen Shi ◽  
...  

1985 ◽  
Vol 51 ◽  
Author(s):  
Y. R. Shen

ABSTRACTThe recent status of applications of nonlinear optics to surface science is reviewed. The basic theory of wave mixing on a surface layer, and the possibility of using various nonlinear optical processes for surface probing are briefly discussed. Emphasis is on surface second harmonic generation, which is shown with many illustrations to be a rather unique and versatile tool for surface studies.


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