1991
DOI: 10.1364/ol.16.001726
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LiB_3O_5: a highly efficient frequency converter for Ti:sapphire lasers

Abstract: Efficient second-harmonic generation in a LiB(3)O(5) crystal over the spectral range of a Ti:sapphire laser is demonstrated. The angular acceptance and damage threshold of the LiB(3)O(5) crystal are measured and calculated, and a 30% conversion efficiency is achieved (with a 5-mm-long crystal). The potential for increasing the conversion efficiency of second-harmonic generation at the edges of the spectral range of the Ti:sapphire laser is shown.

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Cited by 27 publications
(2 citation statements)
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“…The Ti:sapphire laser, which was pumped by a continuous wave (cw) argon ion laser, produced a 840 nm light pulsed of 1.5 ps duration and had a repetition rate of 82 MHz. The third harmonic radiation (THG) was generated by overlapping the fundamental and second harmonic radiation (SHG). , For the THG and SHG crystals, LiIO 3 and BBO were employed, respectively. The pulse repetition rate was decreased to 8.2 MHz by using an electrooptic light modulator (Con Optic, Model 1305).…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The Ti:sapphire laser, which was pumped by a continuous wave (cw) argon ion laser, produced a 840 nm light pulsed of 1.5 ps duration and had a repetition rate of 82 MHz. The third harmonic radiation (THG) was generated by overlapping the fundamental and second harmonic radiation (SHG). , For the THG and SHG crystals, LiIO 3 and BBO were employed, respectively. The pulse repetition rate was decreased to 8.2 MHz by using an electrooptic light modulator (Con Optic, Model 1305).…”
Section: Methodsmentioning
confidence: 99%
“…The third harmonic radiation (THG) was generated by overlapping the fundamental and second harmonic radiation (SHG). 18,19 For the THG and SHG crystals, LiIO 3 and BBO were employed, respectively. The pulse repetition rate was decreased to 8.2 MHz by using an electrooptic light modulator (Con Optic, Model 1305 The overall instrument response function has a full width at half-maximum (fwhm) of approximately 30 ps at the excitation wavelength of 280 nm.…”
Section: Methodsmentioning
confidence: 99%