J. M. Sarraute, K. Schires, S. LaRochelle, F. Grillot, "Effects of gain nonlinearities in an optically injected gain lever semiconductor laser," Photonics Res. 5, 315 (2017)

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- Photonics Research
- Vol. 5, Issue 4, 315 (2017)

Fig. 1. (a) Schematic of the two-section GL laser (framed by black dotted square). Evolution of the material gain with the carrier density in both sections (left). G a , b ′ are the differential gains in each section. (b) Schematic of the OIL configuration.

Fig. 2. MTF of the free-running laser without GL calculated from 5 for ϵ = 0,5 × 10 − 17 , 10 − 16 , a n d 5 × 10 − 16 cm 3 .

Fig. 3. MTF of the OIGL laser calculated from 3 for different values of gain compression ϵ = 0 , 10 − 17 , 5 × 10 − 17 , a n d 10 − 16 cm 3 and with a GL of g = 10 . The injected power and frequency detuning are (a) K = 3.5 , Δ f / f R = 0.97 and (b) K = 8 , Δ f / f R = 3.3 . Red dotted curves represent the MTF for the free-running case assuming no compression and without GL.

Fig. 4. 3 dB bandwidth in the stable-locking region of the OIGL laser with g = 10 and ϵ = 10 − 16 cm 3 .

Fig. 5. Evolution of the 3 dB bandwidth with respect to GL strength and gain compression factor for (a) K = 0 and (b) K = 8 .
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Table 1. Material and Laser Parameters

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