Abstract

A compact second-order Stokes Brillouin fiber laser made of microstructured chalcogenide fiber is reported for the first time. This laser required very low pump power for Stokes conversion: 6 mW for first order lasing and only 30 mW for second order lasing with nonresonant pumping. We also show linewidth-narrowing as well as intensity noise reduction for both the 1st and 2nd order Stokes component when compared to that of the pump source.

Highlights

  • We show linewidth-narrowing as well as intensity noise reduction for both the 1st and 2nd order Stokes component when compared to that of the pump source

  • Brillouin fiber lasers (BFLs) have been attracting a lot of interest lately due to their very narrow linewidth [1] and low intensity [2] and frequency noise [3]. 1st order Stokes (S1) Brillouin ring lasers in silica fibers have been exploited for many applications ranging from microwave photonics applications [4] to gyroscopes [5]

  • This corresponds to a free spectral range (FSR) of 19.9 MHz, which is more than the measured ΔνB of 17.6 MHz, ensuring that only one single longitudinal mode is oscillating inside the cavity

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Summary

Introduction

Brillouin fiber lasers (BFLs) have been attracting a lot of interest lately due to their very narrow linewidth [1] and low intensity [2] and frequency noise [3]. 1st order Stokes (S1) Brillouin ring lasers in silica fibers have been exploited for many applications ranging from microwave photonics applications [4] to gyroscopes [5]. A relatively low laser threshold of 22 mW was obtained for nonresonant pumping in a BFL made of a 3-m long suspended-core As38Se62 chalcogenide fiber [9] This laser had very good intensity and frequency noise characteristics. The purpose of this communication is twofold: first to demonstrate the possibility of making compact BFLs operation on 2nd order Stokes component with a relatively low threshold power (section 3) and, second, to experimentally demonstrate the coherency and intensity noise performances of the S2 component generated in the cavity (sections 4 and 5)

Microstructured GeAsSe chalcogenide fiber
Brillouin laser made of microstructured GeAsSe chalcogenide fiber
Linewidth-narrowing effect in Brillouin ring cavity
Relative intensity noise of the Stokes components
Conclusion

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