Abstract

A CS2-filled Er-doped fiber, which can provide high nonlinearity and gain, low and flat all-normal dispersion profile, low loss and single-mode operation in the wavelength range of 1500-2500 nm, is proposed and analyzed by numerical simulation. When the 1900-nm 0.1-ps initial pulse with a peak power of 30 kW is injected into the active fiber, the generated supercontinuum (SC) spectrum has a double-hump structure in the 1550-nm window and covers about 800-nm wavelength range spanning from 1400 to 2200 nm at -20 dB level. Furthermore, the 1550-nm pulse can be obtained synchronously with the 1900-nm initial pulse when the amplified pulse with a temporal double-peak shape is passed through a band-pass filter with its center wavelength at 1550 nm.

Highlights

  • Supercontinuum generation (SCG) in the all-normal dispersion fiber can be useful for applications such as optical coherence tomography [1], nonlinear microscopy [2], biophotonic [3], and ultra-short pulse generation [4] due to its perfect coherent properties

  • It was demonstrated by numerical simulation that the SCG with an enhancement of pulse energy and spectral flatness can be obtained through an ytterbiumdoped high-nonlinearity normal-dispersion photonic crystal fibers (PCFs) [28]

  • The results indicate that for the pulses propagating inside the CS2-filled Er-doped fiber, an increase in the concentration of the rare-earth ions or pump powers can raise the pulse energy and peak power, but has a negligible influence on the spectral bandwidth, which is mainly dependent on the peak power and duration of the initial pulse, and nonlinear parameter and dispersion of the fiber

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Summary

Introduction

Supercontinuum generation (SCG) in the all-normal dispersion fiber can be useful for applications such as optical coherence tomography [1], nonlinear microscopy [2], biophotonic [3], and ultra-short pulse generation [4] due to its perfect coherent properties. The nonlinear parameter of the fiber can be enhanced further for the all-solid soft glass PCF [14]–[16], air-tellurite PCFs [17], tapered tellurite step-index optical fiber [18], As2Se3 chalcogenide glass triangular-core graded-index PCF [19] and hollow-core silica fibers filled with highly nonlinear liquids such as carbon disulfide (CS2) [20]–[25] and chloroform (CHCl3) [26] In the latter case, the SCG covering from 1064 to beyond 1700 nm with 70-W average output power was demonstrated experimentally using a nonlinear ytterbium-doped fiber amplifier with all-normal dispersion [27].

The Properties of the Active CS2-Filled Fiber
The Dispersion and Nonlinearity in the Fiber
The Loss and Gain in the Fiber
Numerical Simulation of the Supercontinuum Generation
The Case of the 1550-nm Initial Pulse
The Case of the 1900-nm Initial Pulse
Conclusion
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