2006
DOI: 10.1002/0471791598
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Photonics and Lasers

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Cited by 113 publications
(88 citation statements)
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“…The optical-to-optical efficiencies for 4.8 µm emission with pump wavelengths of 3.9, 4.0, 4.1 and 4.15 µm are 22, 37, 51 and 55% respectively. Note that the Stokes efficiency limit for a pump wavelength of 4.15 μm is 86% (Quimby 2006). Moreover, from the results presented in Fig.…”
Section: Resultsmentioning
confidence: 77%
“…The optical-to-optical efficiencies for 4.8 µm emission with pump wavelengths of 3.9, 4.0, 4.1 and 4.15 µm are 22, 37, 51 and 55% respectively. Note that the Stokes efficiency limit for a pump wavelength of 4.15 μm is 86% (Quimby 2006). Moreover, from the results presented in Fig.…”
Section: Resultsmentioning
confidence: 77%
“…The peak intensity for Gaussian beam is two times higher than it is often assumed and this formula can be verified by integrating the intensity over the whole beam area (Quimby 2006). Additionally, assuming that temporal coherence of the exciting source depends only on the duty cycle and the shape of the pulse we can write:…”
Section: Theoretical Considerationmentioning
confidence: 90%
“…Note that in the following, the dye spontaneous lifetime τ sp is defined as the inverse of Einstein A coefficient. This dye spontaneous lifetime τ sp should not be mistaken as the photoluminescence (PL) lifetime τ PL , 39 which is the defined as the product of τ sp and dye quantum efficiency (yield) q dye . Finally, the NrD rate is expressed as N/τnr, where the non-radiative decay lifetime τ nr can be calculated by τ nr = τ sp q dye /(1-q dye ) since…”
Section: Generalized Full Rate Equation Model and Analysismentioning
confidence: 99%