Electro-optic modification of second-harmonic phase-matching spectra in segmented periodically poled LiNbO_3

2002 ◽  
Vol 19 (2) ◽  
pp. 280 ◽  
Author(s):  
Heiko Ridderbusch ◽  
Marvin E. Klein ◽  
Petra Gross ◽  
Dong-Hoon Lee ◽  
Jan-Peter Meyn ◽  
...  
2003 ◽  
Vol 11 (22) ◽  
pp. 2813 ◽  
Author(s):  
Yeung Lak Lee ◽  
Young-Chul Noh ◽  
Changsoo Jung ◽  
Tae Yu ◽  
Do-Kyeong Ko ◽  
...  

2005 ◽  
Vol 44 (26) ◽  
pp. 5561 ◽  
Author(s):  
Rui Wu ◽  
Yuping Chen ◽  
Junfeng Zhang ◽  
Xianfeng Chen ◽  
Yuxing Xia

1991 ◽  
Vol 58 (1) ◽  
pp. 34-35 ◽  
Author(s):  
N. Schmidt ◽  
K. Betzler ◽  
B. C. Grabmaier

2008 ◽  
Vol 47 (8) ◽  
pp. 6777-6783 ◽  
Author(s):  
Solomon M. Saltiel ◽  
Dragomir N. Neshev ◽  
Robert Fischer ◽  
Wieslaw Krolikowski ◽  
Ady Arie ◽  
...  

Author(s):  
Yusuke Hisai ◽  
Yoshiki Nishida ◽  
Hiroshi Miyazawa ◽  
Takumi Kobayashi ◽  
Feng-Lei HONG ◽  
...  

Abstract We demonstrate a second harmonic generation (SHG) of 116 mW at 461 nm in a periodically poled lithium niobate waveguide when the power of the 922-nm fundamental light is coupled into the waveguide was 350 mW. The waveguide is 12.5 μm wide, 12.0 μm thick, 22 mm long, and has a 1-mm-long slab window at the output facet of the waveguide. The temperature acceptance bandwidth of the phase-matching curve of the SHG is approximately 0.5 °C. The SHG system demonstrates good beam quality and is reliable for cold atom experiments, including research on optical lattice clocks.


2020 ◽  
Vol 128 (11) ◽  
pp. 1717
Author(s):  
В.Ю. Мыльников ◽  
Н.С. Аверкиев ◽  
Г.С. Соколовский

We theoretically demonstrate cascaded fourth and second harmonic generation in a periodically-poled nonlinear crystal with a half-order of phase-matching period. We consider a cascaded process in which four photons of the fundamental harmonic firstly convert into an intermediate photon of the fourth harmonic, which parametrically decays into two photons of the second harmonic at the second stage. Phase-matching for this cascaded nonlinear conversion is provided by using an asymmetric periodical poling. We use the quantum spatial Heisenberg equations to describe light propagation and conversion inside the nonlinear crystal. With this approach, we calculate second and fourth harmonic average number of photons as a function of the nonlinear crystal length.


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