2012
DOI: 10.7452/lapl.201210085
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Green-to-red tunable SHG of a quantum-dot laser in a PPKTP waveguide

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Cited by 25 publications
(25 citation statements)
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“…The high-order fundamental and low-order SHG modes are attributed to the frequency doubling on the red side of the tuning range. These results are in excellent agreement with a multimode interaction model very recently presented in [27]. With respect to applications, a Gaussian beam profile is mandatory.…”
Section: Broadly Tunable Frequency-doubled Ec-qd Laserssupporting
confidence: 78%
See 3 more Smart Citations
“…The high-order fundamental and low-order SHG modes are attributed to the frequency doubling on the red side of the tuning range. These results are in excellent agreement with a multimode interaction model very recently presented in [27]. With respect to applications, a Gaussian beam profile is mandatory.…”
Section: Broadly Tunable Frequency-doubled Ec-qd Laserssupporting
confidence: 78%
“…The generated fundamental emission from the gain chip output facet is then focused by high-NA optics into a periodically poled potassium titanyl phosphate (PPKTP) waveguide. To provide a large wavelength range for frequency conversion from a single crystal, a generalization of quasiphase matching (QPM) based on the utilization of a significant difference in the effective refractive indices of the high-and low-order modes in multimode waveguides is studied and realized [27]. This novel approach allows matching the period of poling in a very broad wavelength range and opens up a new avenue for an order-of-magnitude increase in SHG conversion bandwidth with respect to QPM.…”
Section: Broadly Tunable Frequency-doubled Ec-qd Lasersmentioning
confidence: 99%
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“…This 73 nm tunability (not continuous) was achieved by exploiting both the broadband tunability of the fundamental radiation allowed by a multimode QD laser, along with the quasi−phase matching in a multimode waveguided periodically−poled KTP and tapping into the significant difference in the effective refractive indices of the higher and lower−order modes [71], as previously demonstrated in [72]. A maximum power of 12 mW was achieved at 605.6 nm, with an efficiency of 10.3%.…”
Section: Applicationsmentioning
confidence: 92%