Nonlinear control for soliton interactions in optical fiber systems

Zhang, Pei; Hu, Cheng; Zhou, Qin; Biswas, Anjan; Liu, Wenjun

doi:10.1007/s11071-020-05865-3

Cited by 9 publications

(2 citation statements)

References 38 publications

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“…Optical solitons have potential applications in the fields of optical communications and optical information processing. [1][2][3] Passively mode-locked ultrafast fiber laser is often constructed to study soliton dynamics. [4][5][6][7] More often, vector soliton can be generated in fiber laser because the intrinsic linear birefringence of the single-mode fiber, which is brought by strain, temperature variation, and fabrication imperfection.…”

Section: Introductionmentioning

confidence: 99%

“…In theory, the vector soliton in a dissipative fiber laser system can be well described using coupled Ginzburg-Landau equations, which include fiber dispersion, gain, loss, self-phase modulation, cross-phase modulation, coherent energy coupling, gain bandwidth, and so on. [1,6] In experiment, different kinds of vector solitons can be generated through changing intra-cavity linear birefringence and pump power, such as group-velocity-locked vector soliton (GVLVS), [9][10][11] polarization-locked vector soliton (PLVS), [12,13] and polarization rotation vector soliton (PRVS). [14] For GVLVS, the two orthogonal polarization modes will shift their central wavelengths in opposite directions and copropagate as a unit without splitting.…”

Section: Introductionmentioning

confidence: 99%

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Polarization manipulation of bright-dark vector bisolitons*

et al. 2021

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We simulate the polarization manipulation of bright-dark vector bisolitons at 1-μm wavelength regime. Through changing the pulse parameters, different kinds of pulse shapes and optical spectra are generated in output orthogonal polarization directions. When the input vector bisoliton is polarization-locked with 1064 nm central wavelength, “1+1” fundamental dark-dark and “2+1” pseudo-high-order bright-dark group-velocity-locked vector solitons can be achieved through changing the projection angle. When the input vector bisoliton is group-velocity-locked with 1063 nm and 1065 nm central wavelengths, “2+1” and “2+2” pseudo-high-order bright-dark group-velocity-locked vector solitons, bright-dark group-velocity-locked vector solitons with chirp-like temporal oscillations are generated. Our simulation results can provide beneficial conduct for polarization manipulation of vector multi-solitons, and have promising applications in quantum information register, optical communications, nanophotonics, and all-optical switching.

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