Effects of high frequency injection and optical feedback on semiconductor laser performance

1990 ◽  
Author(s):  
Edward C. Gage ◽  
Scott Beckens
Keyword(s):  
Semiconductor Laser ◽  
High Frequency ◽  
Optical Feedback ◽  
Laser Performance

High-frequency optical signal generation in a semiconductor laser by incoherent optical feedback

1998 ◽  
Vol 150 (1-6) ◽  
pp. 158-162 ◽  
Author(s):  
Tsu-Chiang Yen ◽  
Jer-Wei Chang ◽  
Jenn-Ming Lin ◽  
Rong-Jyh Chen
Keyword(s):  
Semiconductor Laser ◽  
High Frequency ◽  
Optical Feedback ◽  
Optical Signal ◽  
Signal Generation

Optical spectra of a semiconductor laser with incoherent optical feedback

1990 ◽  
Vol 26 (6) ◽  
pp. 982-990 ◽  
Author(s):  
J.S. Cohen ◽  
F. Wittgrefe ◽  
M.D. Hoogerland ◽  
J.P. Woerdman
Keyword(s):  
Semiconductor Laser ◽  
Optical Feedback ◽  
Optical Spectra

The Role of Master Laser with Feedback in Time-Delay Signature Suppression of Semiconductor Laser Subject to Chaotic Optical Injection

2017 ◽  
Vol 27 (11) ◽  
pp. 1750169 ◽  
Author(s):  
Liyue Zhang ◽  
Wei Pan ◽  
Penghua Mu ◽  
Xiaofeng Li ◽  
Shuiying Xiang ◽  
...  
Keyword(s):  
Time Delay ◽  
Semiconductor Laser ◽  
Optical Feedback ◽  
Bias Current ◽  
Optical Injection ◽  
Strength Parameter ◽  
Master Laser ◽  
Feedback Strength ◽  
Chaotic Signals

The important role of parameters in master laser with optical feedback for the elimination of time-delay (TD) signature in semiconductor laser subject to chaotic optical injection is investigated systemically. The experimental results show that TD signature suppressed chaotic signals can be credibly generated by increasing the feedback strength of the master laser, which is quite different from the trends observed in semiconductor laser (SL) with optical feedback. Systematically numerical analysis is also carried out as a validation, and it is shown that with low bias current and strong feedback strength, parameter regions contributing to successful TD suppression are much wider. Furthermore, it is shown that the influence of frequency detuning in TD concealment will change with the increase of feedback strength. All the numerical results are in perfect accordance with experimental observation.

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