Abstract

Using numerical simulations of thermally induced mode coupling we show how the instability threshold can be substantially reduced if the pump or injected signal is modulated in the kHz range. We also show how the mode coupling gain varies with the frequency offset of the parasitic mode. We model thresholds when the source of detuned light is quantum background, amplitude modulation of the pump power, and amplitude modulation of the signal seed. We suggest several key experimental and modeling tests of our model.

Highlights

  • In attempts to scale fiber amplifiers to high power, maximizing the modal area has been an effective way to suppress nonlinearities such as stimulated Brillouin and Raman scattering.Due to practical limitations on refractive index control, large mode area fibers typically support several transverse modes, and this makes them susceptible to a modal instability in which some of the light propagating in the desired LP01 mode is transferred into mode LP11

  • We constructed a numerical model of the amplifier and used it to first find an equilibrium solution which, in our case, is a set of signal and pump optical fields defined along the length of the fiber

  • We have explained how instability thresholds can be sensitive to the operating conditions, pump or signal modulations combined with slight initial population of LP11

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Summary

Introduction

In attempts to scale fiber amplifiers to high power, maximizing the modal area has been an effective way to suppress nonlinearities such as stimulated Brillouin and Raman scattering. We present a detailed discussion of this question, showing how our model can account for observed threshold powers as well as a sensitivity to operating conditions. We present details of our improved model along with some key modeling results showing dependence of the threshold on operating conditions - namely on modulation of the input signal seed, modulation of the pump, and accidental launch of signal seed light into mode LP11. These factors can act to initially populate LP′11, and our model can make quantitative predictions of the resulting threshold reductions

Mode coupling mechanism
Model details
Using the ADI method
Using the Green’s function method
Gain spectrum
Model parameters
Quantum noise
Spontaneous thermal Rayleigh scattering
Pump modulation
Signal modulation
Threshold calculations
Comparison with measured thresholds
Look for frequency shifts
Numerical experiments
10. Conclusions
11. Appendix A
Findings
12. Appendix B
Full Text
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