Abstract

We demonstrate the generation of dark pulses from carbon nanotube (CNT) incorporated erbium-doped fiber ring lasers with net anomalous dispersion. A side-polished fiber coated with CNT layer by optically-driven deposition method is embedded into the laser in order to enhance the birefringence and nonlinearity of the laser cavity. The dual-wavelength domain-wall dark pulses are obtained from the developed CNT-incorporated fiber laser at a relatively low pump threshold of 50.6 mW. Dark pulses repeated at the fifth-order harmonic of the fundamental cavity frequency are observed by adjusting the intra-cavity polarization state.

Highlights

  • Dark pulse operation of lasers has emerged as an attractive topic in laser physics with respect to bright pulses in recent years [1, 2]

  • We demonstrate the generation of dark pulses from carbon nanotube (CNT) incorporated erbium-doped fiber ring lasers with net anomalous dispersion

  • A side-polished fiber coated with CNT layer by optically-driven deposition method is embedded into the laser in order to enhance the birefringence and nonlinearity of the laser cavity

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Summary

Introduction

Dark pulse operation of lasers has emerged as an attractive topic in laser physics with respect to bright pulses in recent years [1, 2]. The mechanism of fiber lasers with net anomalous dispersion to produce dark pulses can be explained by domain-wall theory, in which two leasing beams originated from two-Eigen operation states of fiber lasers are coupled incoherently with each other [7]. Such two-Eigen operation states of lasers can be achieved by managing either the two orthogonal polarization states of the lasers or two separated wavelengths induced by intra-cavity birefringent filter [1, 8]. Theoretical studies have predicted that the nonlinearity of CNTs is almost eight-order magnitude larger than that of standard single mode fiber [12], and recent demonstrations have confirmed that a very short-length of CNTdeposited device has a comparable Kerr nonlinearity to a relative long-length of highly nonlinear fiber [14, 15]

Methods
Conclusion

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