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Modeling of gain and phase dynamics in quantum dot amplifiers

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Academic year: 2021

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Figure

Fig. 1 Energy discretization of the GS and ES 0.8 0.9 1 1.1 1.200.511.52x 1013DOS (eV-1 cm-2) Energy (eV) E iESGS
Fig. 2 Intradot mechanisms considered in the rate equations
Fig. 3 Change of the gain at the GS peak after the arrival of the pump at t = 0. The current injection of the amplifier is 0 mA.
Fig. 4 Phase shift at the GS peak energy, under no injected current (0 mA). Note that the left side is plotted in linear scale and the right side in logarithmic (x-axis)
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