1997
DOI: 10.1364/ol.22.001302
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Fourth-harmonic generation of a continuous-wave CO_2 laser by use of an AgGaSe_2/ZnGeP_2 doubly resonant device

Abstract: We report a doubly resonant continuous-wave CO(2) laser frequency-quadrupling device that generates 200nW of 2.55-mum (4?) and as much as 2mW of 5.1-mum (2?) radiation out of 1.7-W fundamental radiation at 10.2 mum (?). The quadrupling process results from two resonant cascading second-harmonic generations by use of a walk-off-compensated twin AgGaSe(2) device (??2?) and a ZnGeP(2)nonlinear crystal (2??4?).

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Cited by 19 publications
(4 citation statements)
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“…The performance of devices based on mid-IR chalcogenides is often limited by deleterious thermal effects (lensing, expansion) [4,7,24]. The thermal figure of merit of a material can be defined by the quantity η = (dn/dT )/K where dn/dT is the thermo-optic index variation and K is the thermal conductivity.…”
Section: Thermal and Thermo-optic Propertiesmentioning
confidence: 99%
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“…The performance of devices based on mid-IR chalcogenides is often limited by deleterious thermal effects (lensing, expansion) [4,7,24]. The thermal figure of merit of a material can be defined by the quantity η = (dn/dT )/K where dn/dT is the thermo-optic index variation and K is the thermal conductivity.…”
Section: Thermal and Thermo-optic Propertiesmentioning
confidence: 99%
“…The thermally-related properties of a new nonlinear material are crucial in assessing its potential in real nonlinear conversion devices pumped by high power cw or pulsed lasers. The performance of devices based on mid-IR chalcogenides is often limited by deleterious thermal effects (lensing, expansion) [4,7,24]. The thermal figure of merit of a material can be defined by the quantity η = (dn/dT )/K where dn/dT is the thermo-optic index variation and K is the thermal conductivity.…”
Section: Thermal and Thermo-optic Propertiesmentioning
confidence: 99%
See 1 more Smart Citation
“…In this case, integration is less important, and the key technological task is the development of high-intensity lasers operating at wavelengths in the mid-(3 − 5µm) and far-IR (8 − 12µm). [2][3][4][5][6] The limitations imposed by the transparency windows of the earth's atmosphere in such high power applications do not apply to the highly-localized SSMS systems, which generally provides for a wider range of detection.…”
mentioning
confidence: 99%