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Lasing from active optomechanical resonators

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Figure

Fig. 1c). This excellent agreement between measured andcalculated frequencies demonstrates that the laser emission is
Figure 2 | Modulation of the lasing output in VCSEL1. ((temporal zones A–E. Zones C and E correspond to the ranges in which long-living resonant phonons of the active optomechanical device persist in thecavity layer containing the optically active medium
Figure 4 | Deformation potential mechanism for VCSEL1. (a) Calculatedtemporal evolution of the sum of the strain applied to all 12 QWs

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