Novel D-π-A-π-D type organic chromophores for second harmonic generation and multi-photon absorption applications

2013 ◽  
Author(s):  
Pusala Aditya ◽  
Hari Kumar ◽  
Sunil Kumar ◽  
Rajashekar ◽  
M. Muralikrishna ◽  
...  
Nanoscale ◽  
2019 ◽  
Vol 11 (37) ◽  
pp. 17293-17300 ◽  
Author(s):  
Michael T. Quick ◽  
Nina Owschimikow ◽  
Ali Hossain Khan ◽  
Anatolii Polovitsyn ◽  
Iwan Moreels ◽  
...  

We investigate broadband two-photon absorption autocorrelators based on II–VI semiconductor nanoplatelets as an alternative to common second harmonic generation based techniques.


1999 ◽  
Vol 24 (11) ◽  
pp. 756 ◽  
Author(s):  
Todd G. Ulmer ◽  
Ronson K. Tan ◽  
Zhiping Zhou ◽  
Stephen E. Ralph ◽  
Richard P. Kenan ◽  
...  

2004 ◽  
Vol 14 (15) ◽  
pp. 2443 ◽  
Author(s):  
Yue-zhi Cui ◽  
Qi Fang ◽  
Zhen-li Huang ◽  
Gang Xue ◽  
Gui-bao Xu ◽  
...  

Crystals ◽  
2019 ◽  
Vol 9 (7) ◽  
pp. 365 ◽  
Author(s):  
Dam Thuy Trang Nguyen ◽  
Ngoc Diep Lai

We investigate theoretically and experimentally the creation of virtually any polymer-based photonic structure containing individual nonlinear KTiOPO 4 nanoparticles (KTP NPs) using low one-photon absorption (LOPA) direct laser writing (DLW) technique. The size and shape of polymeric microstructures and the position of the nonlinear KTP crystal inside the structures, were perfectly controlled at nanoscale and on demand. Furthermore, we demonstrated an enhancement of the second-harmonic generation (SHG) by a factor of 90 when a KTP NP was inserted in a polymeric pillar. The SHG enhancement is attributed to the resonance of the fundamental light in the cavity. This enhancement varied for different KTP NPs, because of the random orientation of the KTP NPs, which affects the light/matter interaction between the fundamental light and the NP as well as the collection efficiency of the SHG signal. The experimental result are further supported by a simulation model using Finite-Difference Time-Domain (FDTD) method.


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