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1977
DOI: 10.1007/bf00886039
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Resonance amplifier model describing diode lasers coupled to short external resonators

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Cited by 41 publications
(8 citation statements)
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“…where R e = |r e | 2 relates the power reflectivity to the complex field reflectivity r e . We use the model for the effective reflectivity by Voumard et al [33], detailed further in the Supplemental Material [34]. Neglecting phase components, at threshold, R 1 R e e ( g−α t )2L = 1, where g = g th is the (threshold) gain coefficient.…”
Section: A External Cavity Laser Modelmentioning
confidence: 99%
“…where R e = |r e | 2 relates the power reflectivity to the complex field reflectivity r e . We use the model for the effective reflectivity by Voumard et al [33], detailed further in the Supplemental Material [34]. Neglecting phase components, at threshold, R 1 R e e ( g−α t )2L = 1, where g = g th is the (threshold) gain coefficient.…”
Section: A External Cavity Laser Modelmentioning
confidence: 99%
“…where R e = |r e | 2 relates the power reflectivity to the complex field reflectivity, r e . We use the model for the effective reflectivity by Voumard et al [32], detailed further in the Supplementary Information. Neglecting phase components, at threshold R 1 R e e (Γg−αt)2L = 1, where g = g th is the (threshold) gain coefficient.…”
Section: A External Cavity Laser Modelmentioning
confidence: 99%
“…The solution of (14) indicates that the population inversion increases with current density until threshold is reached. At that point, N approaches its asymptotic value N t h = y/o.…”
Section: Laser Output Characteristicsmentioning
confidence: 99%