Finite-size effects on squeezing in the self-pulsing regime of second harmonic generation

1997 ◽  
Vol 55 (6) ◽  
pp. 4516-4519 ◽  
Author(s):  
Oliver Veits ◽  
Michael Fleischhauer
2019 ◽  
Vol 126 (6) ◽  
pp. 724
Author(s):  
А.А. Шамына ◽  
В.Н. Капшай

In the Rayleigh–Gans–Debye approximation an analytical solution is obtained for the problem of second harmonic generation by a plane electromagnetic wave with elliptical polarization from a thin optically nonlinear layer on the surface of a cylindrical dielectric particle of finite size placed in a dielectric. The result is presented in tensor and vector forms in general case, in which the nonlinear dielectric susceptibility tensor has four independent components (one chiral and three non-chiral). For the first time it is shown that at generation from the end plane surfaces of a cylindrical particle the contribution of chiral components differs in phase from that of non-chiral components. It is also found that for small linear dimensions of the cylindrical particle (height and radius of the base), the radiation due to the chiral component of the second-order nonlinear dielectric susceptibility tensor makes a dominant contribution to the second harmonic generation from a non-linear cylindrical layer (end and side surfaces).


1997 ◽  
Vol 78 (1) ◽  
pp. 46-49 ◽  
Author(s):  
O. A. Aktsipetrov ◽  
A. A. Fedyanin ◽  
E. D. Mishina ◽  
A. A. Nikulin ◽  
A. N. Rubtsov ◽  
...  

2001 ◽  
Vol 13 (10) ◽  
pp. 2211-2224 ◽  
Author(s):  
P D Townsend ◽  
A K Jazmati ◽  
T Karali ◽  
M Maghrabi ◽  
S G Raymond ◽  
...  

Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Jicheng Jin ◽  
Jian Lu ◽  
Bo Zhen

Abstract Second harmonic generation through nonlinear nano-photonic structures is important in both classical and quantum applications. It is commonly expected that the second harmonic frequency can always be generated as long as appropriate quadratic nonlinearity is provided by the material and the phase-matching condition is satisfied. Here, we present an anomaly to this common wisdom by showing that second-harmonic dipoles generated in a nonlinear photonic crystal slab can be completely nonradiative. As a result, no energy is transferred from the fundamental frequency to the second harmonic even when the phase-matching condition is satisfied – a phenomenon we call “resonance-forbidden second-harmonic generation”. Through numerical simulation, we identify two mechanisms that can achieve this phenomenon: symmetry protection and parameter tuning. The finite-size effect and the topological origin of this phenomenon are also discussed.


2020 ◽  
Vol 101 (10) ◽  
Author(s):  
Yi-Zen Chu ◽  
Klaountia Pasmatsiou ◽  
Glenn D. Starkman

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