2001
DOI: 10.1364/ol.26.001961
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Efficient frequency doubling of a pulsed laser diode by use of a periodically poled KTP waveguide crystal with Bragg gratings

Abstract: Blue light with an average power of as much as 7.5 mW in picosecond pulses has been generated at 486, 488, and 491 nm from a frequency-doubled, nonresonant injection seeded, gain-switched InGaAs/GaAs diode laser by use of a periodically poled KTP waveguide crystal that incorporates a Bragg grating section.

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Cited by 24 publications
(12 citation statements)
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“…The resonator was formed between the diode laser back facet and the rear facet of the nonlinear crystal. At gain switched operation, it was possible to generate light at a wavelength of 486 nm with 7.5 mW average power out of 144 mW fundamental power [159].…”
Section: Intracavity Shg Using Diode Lasersmentioning
confidence: 99%
“…The resonator was formed between the diode laser back facet and the rear facet of the nonlinear crystal. At gain switched operation, it was possible to generate light at a wavelength of 486 nm with 7.5 mW average power out of 144 mW fundamental power [159].…”
Section: Intracavity Shg Using Diode Lasersmentioning
confidence: 99%
“…Small beam divergence angle is favored to reduce the coupling loss between the laser and the optics, can simplify the optical system enabling direct coupling to fiber and, finally, increase the delivered optical power. Reducing beam divergence below 2-4 degrees will open up new exciting opportunities for external cavity applications and direct frequency conversion using edge-emitting lasers, an approach demonstrated for VCSELs [2]. Multimode operation.…”
Section: Introductionmentioning
confidence: 99%
“…10that both well-defined facets of the corrugated interfaces and the related natural compositional superlattice are wellRefractive index profile (thin solid line), absolute value of the electric field strength of the fundamental mode TE 1 (thick solid line) and higher-order mode TE 2 (thick dashed line) (lefthand side column) and vertical far-field intensity pattern of the fundamental mode TE 1 (right-hand side column) for four (first row), eight (second row) and twelve (third row) high-refractive index layers and the low-refractive index layers and wavelength 646 nm. In the left-hand side column the relative optical confinement factors Γ are given for lowest-order modes TE[1][2][3][4] .…”
mentioning
confidence: 99%
“…For efficient frequency conversion this pump source has to have a narrow spectral line width. At low power levels up to 500 mW low cost commercially available ridge waveguide (RW) lasers with an external frequency selective Bragg grating were used as pump source for SHG [2]. There an average output power of 7.5 mW at 486, 488, and 491 nm was generated in a PPKTP waveguide crystal in a picosecond pulse mode.…”
Section: Introductionmentioning
confidence: 99%