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Simulation of optical fiber power amplification via higher-order soliton generation using the extended nonlinear Schrödinger equation

2025Open accessBenue State University

In plain language

Numerical simulations investigate optical fibre power amplification through the generation of higher-order solitons. An extended nonlinear Schrödinger equation was solved using the split-step Fourier method, applying multi-peaked Gaussian functionals as initial conditions while varying parameters of loss, group velocity dispersion, and nonlinearity. Increasing group velocity dispersion from 0.05 to 0.1 fs/nm.km generates higher-order solitons across all orders, broadening the pulse and boosting peak power from 4.5309 W for first-order solitons to 14.9508 W for second-order and 15.0828 W for third-order solitons. This amplification occurs because newly formed solitons draw energy from radiation within dispersed pulses despite overall optical power attenuation. Conversely, raising loss, dispersion, and nonlinearity coefficients simultaneously between 0.1 and 1.0 causes persistent power attenuation, resulting in noisy signal radiation that scatters and decays exponentially over short propagation distances.

Key takeaways

  • Increasing group velocity dispersion from 0.05 to 0.1 fs/nm.km enables the formation of higher-order solitons.
  • Peak soliton power increases from 4.5309 W in the first order to 15.0828 W in the third order.
  • Newly generated solitons gain power by absorbing energy from the radiation present in dispersed solitons.
  • Simultaneously increasing loss, dispersion, and nonlinearity coefficients from 0.1 to 1.0 produces signal radiation that scatters and decays exponentially.

Why it matters

Understanding how light pulses behave and amplify inside optical fibres is essential for managing signal strength and noise in optical transmission. By demonstrating how higher-order solitons can harness dispersed energy to increase peak power, these simulation findings clarify the specific dispersion and loss thresholds needed to sustain signal integrity without triggering destructive noise and signal decay.

Commercialisation angle

The abstract does not indicate a direct commercial application pathway, presenting early-stage numerical simulation research. The findings could potentially inform engineers developing optical communication equipment or fibre laser systems on dispersion settings, but the work remains at the computational modelling stage and is distant from real-world physical deployment.

AI-generated from the published abstract. Always read the original work before citing.

Abstract

This study seeks to simulate the amplification of the optical fiber power by the generation of higher order solitons. This was achieved by solving an extended form of the nonlinear Schrödinger equation (NLSE) using the split step Fourier method (SSFM) with Gaussian functionals having multiple peaks as initial conditions to simulate the generation of higher order solitons in the optical fiber. Some key fiber parameters such as the coefficients of loss α, group velocity dispersion β and nonlinearity γ were varied and the respective effects on the optical fiber and soliton power were then observed using spatial plots, 3-D contour plots and image color maps. Results obtained showed that in all soliton orders, higher order solitons were created when β was increased from 0.05 to 0.1 fs/nm.km. This shows a broadening of the soliton to create higher order solitons when dispersion is managed within that range which results in a boost in the peak soliton power amplified from 4.5309 W to 14.9508 W and then to 15.0828W as the soliton order was increased from 1st – 2nd – 3rd order respectively using Gaussian functionals. The extra power gained is as a result of the fact that a newly created soliton takes its energy from the radiation present in the dispersed soliton even though the optical power attenuates. It was also observed that, increasing the coefficients α, β and γ from 0.1 – 1.0 results in a continuous attenuation of the optical fiber power leading to the propagation of radiation (noisy signal) in the optical fiber which scatters and exponentially decays after a short distance along the length of the optical fiber.

Research topics

  • Optical Network Technologies
  • Advanced Fiber Laser Technologies
  • Photonic Crystal and Fiber Optics

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DOI: 10.61298/rans.2025.3.1.152

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