Abstract

The capacity and reach of long-haul fiber optical communication systems is limited by in-line amplifier noise and fiber nonlinearities. Phase-sensitive amplifiers add 6 dB less noise than conventional phase-insensitive amplifiers, such as erbium-doped fiber amplifiers, and they can provide nonlinearity mitigation after each span. Realizing a long-haul transmission link with in-line phase-sensitive amplifiers providing simultaneous low-noise amplification and nonlinearity mitigation is challenging and to date no such transmission link has been demonstrated. Here, we demonstrate a multi-channel-compatible and modulation-format-independent long-haul transmission link with in-line phase-sensitive amplifiers. Compared to a link amplified by conventional erbium-doped fiber amplifiers, we demonstrate a reach improvement of 5.6 times at optimal launch powers with the phase-sensitively amplified link operating at a total accumulated nonlinear phase shift of 6.2 rad. The phase-sensitively amplified link transmits two data-carrying waves, thus occupying twice the bandwidth and propagating twice the total power compared to the phase-insensitively amplified link.

Highlights

  • PSAs can be realized, for example using, parametric gain in χ(2) nonlinear materials through three-wave mixing (TWM)[11], or χ(3) nonlinear materials through four-wave mixing (FWM)[12]

  • We present experimental evidence that in-line PSAs, can provide an unprecedented nonlinear tolerance and transmission reach extension[9,10]. In this demonstration of a recirculating loop transmission experiment with in-line PSAs, we benefit from the inherent simultaneous low-noise amplification and nonlinearity mitigation. This scheme, which is both modulation format-independent and multi-channel compatible[5], is shown experimentally to have a 5.6 times reach improvement compared to a transmission link using conventional in-line erbium-doped fiber amplifiers (EDFAs) when transmitting a 10 GBd quadrature phase-shift keying (QPSK) signal

  • Where us,i are the signal and idler wave amplitudes, ns,i represents vacuum noise present at the input, and the amplifier is characterized via the scalar coefficients μ and ν, where jμj2Àjνj21⁄4 1 ensures photon-number conservation, i.e., two pump photons are converted into one signal and one idler photon

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Summary

Introduction

PSAs can be realized, for example using, parametric gain in χ(2) nonlinear materials through three-wave mixing (TWM)[11], or χ(3) nonlinear materials through four-wave mixing (FWM)[12]. Using other PSA-based schemes, regeneration of more advanced modulation formats such as quadrature phase-shift keying (QPSK)[18,19], and star 8-quadrature amplitude modulation (QAM)[20], have been demonstrated as well as simultaneous regeneration of more than one channel[21,22] Another way to benefit from PSAs is to utilize their capabilities of low-noise amplification and nonlinearity mitigation. In this demonstration of a recirculating loop (i.e., long-haul) transmission experiment with in-line PSAs, we benefit from the inherent simultaneous low-noise amplification and nonlinearity mitigation This scheme, which is both modulation format-independent and multi-channel compatible[5], is shown experimentally to have a 5.6 times reach improvement compared to a transmission link using conventional in-line erbium-doped fiber amplifiers (EDFAs) when transmitting a 10 GBd QPSK signal. The concept of amplification using cascaded PSAs might find applications in the field of quantum information science, where generation and processing of quantum states are of interest

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