Abstract

We experimentally demonstrate optical clock recovery from quantum dot mode-locked semiconductor lasers by interband optical pulse injection locking. The passively mode-locked slave laser oscillating on the ground state or the first excited state transition is locked through the injection of optical pulses generated via the opposite transition bands, i.e. the first excited state or the ground state transition from the hybridly mode-locked master laser, respectively. When an optical pulse train generated via the first excited state from the master laser is injected to the slave laser oscillating via ground state, the slave laser shows an asymmetric locking bandwidth around the nominal repetition rate of the slave laser. In the reverse injection case of, i.e. the ground state (master laser) to the first excited state (slave laser), the slave laser does not lock even though both lasers oscillate at the same cavity frequency. In this case, the slave laser only locks to higher injection rates as compared to its own nominal repetition rate, and also shows a large locking bandwidth of 6.7 MHz.

Highlights

  • Injection locking of semiconductor lasers has been considered as an effective technique to control lasers both in the frequency and time domains

  • We experimentally demonstrate optical clock recovery from quantum dot mode-locked semiconductor lasers by interband optical pulse injection locking

  • When an optical pulse train generated via the first excited state from the master laser is injected to the slave laser oscillating via ground state, the slave laser shows an asymmetric locking bandwidth around the nominal repetition rate of the slave laser

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Summary

Introduction

Injection locking of semiconductor lasers has been considered as an effective technique to control lasers both in the frequency and time domains. The pulse characteristics of quantum dot based mode-locked lasers operating exclusively on the ground state and the excited state transitions have been studied for a two band clock recovery source for telecommunication application [10]. We have experimentally observed that optical pulse injection locking between a master and a slave laser is possible when a master and a slave laser oscillate via different states, e.g., using either GS or ES transitions. An optical pulse train generated from the master laser oscillating on the opposite transition (GS or ES) with respect to the slave laser (ES or GS) is injected into the saturable absorber of the slave laser. Experimental details and results are discussed in the subsequent sections

ES optical pulse injection to the slave laser oscillating via GS transition
GS optical pulse injection to the slave laser oscillating via ES transition
Conclusion
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