Generation of dual-wavelength pulses by frequency doubling with quasi-phase-matching gratings

2001 ◽  
Vol 26 (5) ◽  
pp. 268 ◽  
Author(s):  
G. Imeshev ◽  
M. M. Fejer ◽  
A. Galvanauskas ◽  
D. Harter
1998 ◽  
Vol 150 (1-6) ◽  
pp. 235-238 ◽  
Author(s):  
Xu Guang Huang ◽  
Michael R. Wang

2014 ◽  
Vol 105 (14) ◽  
pp. 141115 ◽  
Author(s):  
A. Majkić ◽  
M. Zgonik ◽  
A. Petelin ◽  
M. Jazbinšek ◽  
B. Ruiz ◽  
...  

2012 ◽  
Vol 32 (3) ◽  
pp. 0319001 ◽  
Author(s):  
郭善龙 Guo Shanlong ◽  
韩亚帅 Han Yashuai ◽  
王杰 Wang Jie ◽  
杨保东 Yang Baodong ◽  
何军 He Jun ◽  
...  

2012 ◽  
Vol 529 ◽  
pp. 81-86 ◽  
Author(s):  
Dong Huang ◽  
Yu Qing Wang ◽  
Jian Yi Luo

We proposed a method to simultaneously implement birefringence-phase-matching (BPM) and quasi-phase-matching (QPM) second harmonic generation (SHG) and polarization coupling including six mismatches of wave vectors, in general case, in an optical superlattice (OSL). And the numerical simulations of SHG and polarization coupling in the OSL are carried out. The results indicate that unlike those of SHG processes with only one second harmonic (SH) reported, when one e-polarized fundamental pump is injected into the OSL, another o-polarized fundamental wave, an o-polarized and an e-polarized SHs can be simultaneously generated. The magnitudes of the o-polarized fundamental wave and SHs can be manipulated by an external dc electric field, which is useful when frequency conversion and signal tuning are required simultaneously.


2001 ◽  
Vol 26 (9) ◽  
pp. 614 ◽  
Author(s):  
L. Gallmann ◽  
G. Steinmeyer ◽  
U. Keller ◽  
G. Imeshev ◽  
M. M. Fejer ◽  
...  

1995 ◽  
Vol 401 ◽  
Author(s):  
J. J. Kingston ◽  
F. Armani-Leplingard ◽  
D. K. Fork ◽  
G. B. Anderson

AbstractThin films of LiNbO3 and LiTaO3 are grown by off-axis magnetron sputtering on A12O3 and LiTaO3 substrates. When stoichiometry is precisely controlled, the films display excellent crystallographic and morphologic properties and have optical losses that are acceptable for frequency-doubling. LiNbO3/A12O3 samples have rocking curve widths as low as Δω = 76 arc sec and rms surface roughnesses less than 1 nm. Rocking curves performed with a resolution of 12 arc sec in 2θ indicate that there is very little tilt to the grains. Most of the width of the standard rocking curve is associated with variations in the interplanar spacing. The LiTaO3 films have similar characteristics. LiNbO3/LiTaO3 samples have rocking curve widths as low as Δω = 28 arc sec. Again, there is very little tilt misalignment to the grains, and the best samples have rms surface roughnesses less than 1 nm. The LiNbO3/LiTaO3 samples are typically 650 nm thick and many have optical losses less than 5 dB/cm. The LiNbO3/A12O3 samples, typically 250 nm thick, have losses of 5–7 dB/cm. The higher modal intensity at the surface of the thinner films increases surface scattering losses.We have generated green light by frequency doubling in LiTaO3 and LiNbO3 thin-film planar waveguides. Phase matching was achieved by both modal dispersion and quasi-phase matching.


2004 ◽  
Vol 68 (6) ◽  
pp. 804-810 ◽  
Author(s):  
Boqin Ma ◽  
Ting Wang ◽  
Peigen Ni ◽  
Bingying Cheng ◽  
Daozhong Zhang

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