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- W3204783162 abstract "In spite of its early discovery in 1965 [1], the passive mode locking of lasers is still a subject of intense research. A type of nonlinear cavity has appeared over the past decade, the so-called mode-locked integrated external-cavity surface-emitting laser (MIXSEL) [2], in which both the gain and the saturable absorber share the same microcavity. In this contribution, we show that due to third-order dispersion from the Gires-Tournois-interferometer-like microcavity, pulses can have a series of decaying satellites on the leading edge [5]. The schematic setup of a MIXSEL system is depicted in Fig. 1 (a). We consider the case of a resonant cavity and we denote the microcavity field over an antinode by E and the field in the external cavity impinging on the top distributed Bragg reflector by Y. After normalization, one obtains the rate equations for the field E, the gain N <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>1</inf> , and the absorber N <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>2</inf> population inversions as follows [3],[4]:begin{align*} & dot E = left[ {left( {1 - i{alpha _1}} right){N_1} + left( {1 - i{alpha _2}} right){N_2} - 1} right]E + hYtag{1} & {dot N_1} = {gamma _1}left( {{J_1} - {N_1}} right) - |E{|^2}{N_1},quad {dot N_2} = {gamma _2}left( {{J_2} - {N_2}} right) - s|E{|^2}{N_2}tag{2} & Y = eta O(t - tau ) = eta [E(t - tau ) - Y(t - tau )].tag{3}end{align*}" @default.
- W3204783162 created "2021-10-11" @default.
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- W3204783162 date "2021-06-21" @default.
- W3204783162 modified "2023-10-02" @default.
- W3204783162 title "Dispersive Instabilities In Passively Mode-Locked Integrated External-Cavity Surface-Emitting Lasers" @default.
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- W3204783162 doi "https://doi.org/10.1109/cleo/europe-eqec52157.2021.9542124" @default.
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