2009
DOI: 10.1007/s00340-008-3359-x
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Electrically controlled second harmonic generation of circular polarization in a single LiNbO3 optical superlattice

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Cited by 6 publications
(2 citation statements)
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“…Not only single optical parametric processes, such as SHG [1][2][3], sum-frequency generation (SFG) [4], and optical parametric oscillation (OPO) [5,6], but also coupled parametric processes, and notably third-harmonic generation [7][8][9], have been achieved in these materials with high efficiency. In recent years, cascaded frequency conversion and electro-optic (EO) coupling (or polarization coupling) have received much research attention [10][11][12][13][14][15][16][17][18][19][20]. We found in these cases only two or three mismatches of wave vector were compensated, which were only special cases included in our united theory [16], however the general case including six mismatches of wave vector is still unsolved.…”
mentioning
confidence: 89%
“…Not only single optical parametric processes, such as SHG [1][2][3], sum-frequency generation (SFG) [4], and optical parametric oscillation (OPO) [5,6], but also coupled parametric processes, and notably third-harmonic generation [7][8][9], have been achieved in these materials with high efficiency. In recent years, cascaded frequency conversion and electro-optic (EO) coupling (or polarization coupling) have received much research attention [10][11][12][13][14][15][16][17][18][19][20]. We found in these cases only two or three mismatches of wave vector were compensated, which were only special cases included in our united theory [16], however the general case including six mismatches of wave vector is still unsolved.…”
mentioning
confidence: 89%
“…It is important to investigate the influence of the domain errors of the APLN crystal on the performance of the filter as the errors are uncontrollable in the fabrication process. The method is the same as that in [21]. We keep E y = 0.219 kV mm −1 , T = 298 K, and L = 8 cm unchanged, and then introduce a pair of positive and negative random errors of length, with the same absolute value and within the range of 0-R, for each couple of adjacent crystal blocks with opposite polarization.…”
Section: Theory and Applicationmentioning
confidence: 99%