Second-harmonic generation and electronic structure of polymethineimines: a theoretical study

1991 ◽  
Vol 176 (2) ◽  
pp. 217-224 ◽  
Author(s):  
I.D.L. Albert ◽  
Puspendu K. Das ◽  
S. Ramasesha
Laser Physics ◽  
2018 ◽  
Vol 28 (2) ◽  
pp. 025404 ◽  
Author(s):  
Jiandong Zhang ◽  
Jian Jiang ◽  
Kai Wang ◽  
Xuan Xiao ◽  
Siyao Yu ◽  
...  

2016 ◽  
Vol 24 (11) ◽  
pp. 11539 ◽  
Author(s):  
Yang-yang Yue ◽  
Han Xiao ◽  
Bo Yang ◽  
Rong-er Lu ◽  
Xu-hao Hong ◽  
...  

2013 ◽  
Vol 12 (02) ◽  
pp. 1250118 ◽  
Author(s):  
JING WEI ◽  
JIN-YUN WANG ◽  
MIN-YI ZHANG ◽  
GUO-LIANG CHAI ◽  
CHEN-SHENG LIN ◽  
...  

The second harmonic generation (SHG) hyperpolarizabilities of phenylalanine and homopolypeptides are investigated by configuration interaction among singly excited configurations (CIS) technique combined with the sum-over-states (SOS) method. The geometries of peptides containing phenylalanine ( Phe )n(n = 1–8) are optimized by B3LYP/6-31g(d) method, and they form the special structures like β-sheet (a common protein secondary structure). It is found that the energy gaps of various peptides are reduced and the hyperpolarizabilities are increased with the peptide chains lengthened. We discuss the origin of the second-order nonlinear optical response in phenylalanine homopolypeptides and confirm that the π → π* transitions in the aromatic residue of phenylalanine make the most important contributions to the second-order polarizability. Our results strongly suggest that the hyperpolarizabilities are dominated from the propagation direction of peptide chains.


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