Theory of second harmonic generation in focused light beam of fundamental frequency with the Gaussian distribution of light intensity under the interaction of type o+o→e

1974 ◽  
Vol 24 (1) ◽  
pp. 1-23 ◽  
Author(s):  
P. Chmela
2009 ◽  
Vol 36 (8) ◽  
pp. 2099-2103
Author(s):  
雷亮 Lei Liang ◽  
陈丽 Chen Li ◽  
胡正发 Hu Zhengfa ◽  
周金运 Zhou Jinyun ◽  
胡义华 Hu Yihua

2014 ◽  
Vol 2014 ◽  
pp. 1-7
Author(s):  
Renlong Zhou ◽  
Mengxiong Wu ◽  
Hui Deng ◽  
Qiong Liu ◽  
Suxia Xie ◽  
...  

Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second-harmonic generation with conversion efficiencies 10−6-10−7. The distributions of fundamental frequency electric field and second-harmonic electric field inside the central dielectric layer region are also shown.


2007 ◽  
Vol 35 (4) ◽  
pp. 273-276
Author(s):  
Hiroshi ISHIJIMA ◽  
Kyoya FUKUDA ◽  
Kensuke MATSUBARA ◽  
Mizuhiko HOSOKAWA

2018 ◽  
Vol 30 (6) ◽  
pp. 064004 ◽  
Author(s):  
Wuyun Shang ◽  
Fajun Xiao ◽  
Lei Han ◽  
Malin Premaratne ◽  
Ting Mei ◽  
...  

2011 ◽  
Vol 217-218 ◽  
pp. 549-554
Author(s):  
Xue Xi Gao ◽  
Wen Jun Wang ◽  
Yun Long Liu ◽  
Yun Li

The poling conditions were studied in AOP process by second harmonic generation (SHG) for host-guest adulterant thin-films. The guest was 4’-Nitro-4-dimethylaminoazobenzene and host was PMMA. The experimental results showed that the optimal poling temperature was about room temperature, the optimal ratio of light intensity of fundamental signal (ω) and its second harmonic signal (2ω) during AOP was approximately 100, the thin films had the same rule that the saturated value of SHG depended on the ratio. In addition, we obtained a suitable thickness around 2200nm that the stronger SHG after poling was generated.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Shukei Sugita ◽  
Takuya Suzumura ◽  
Akinobu Nakamura ◽  
Shinya Tsukiji ◽  
Yoshihiro Ujihara ◽  
...  

AbstractThe ratio of type III to type I collagen is important for properly maintaining functions of organs and cells. We propose a method to quantify the ratio of type III to total (type I + III) collagen (λIII) in a given collagen fiber bundle using second harmonic generation (SHG) light. First, the relationship between SHG light intensity and the λIII of collagen gels was examined, and the slope (k1) and SHG light intensity at 0% type III collagen (k2) were determined. Second, the SHG light intensity of a 100% type I collagen fiber bundle and its diameter (D) were measured, and the slope (k3) of the relationship was determined. The λIII in a collagen fiber bundle was estimated from these constants (k1-3) and SHG light intensity. We applied this method to collagen fiber bundles isolated from the media and adventitia of porcine thoracic aortas, and obtained λIII = 84.7% ± 13.8% and λIII = 17.5% ± 15.2%, respectively. These values concurred with those obtained with a typical quantification method using sodium dodecyl sulfate–polyacrylamide gel electrophoresis. The findings demonstrated that the method proposed is useful to quantify the ratio of type III to total collagen in a collagen fiber bundle.


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