Abstract

Transceiver imperfections become the primary source of impairment as baud rate and modulation order grow in advanced optical coherent communications. Thus, transceiver imperfections, both linear and nonlinear, need to be appropriately characterized, measured, and specified. Treatments for linear imperfections are relatively mature. This study reviews the transceiver's linear imperfection modeling, characterization, and measurement technologies. In practical applications, in-field measurement using the transceiver and a few low speed additional devices is preferred. In the case of nonlinear imperfections, the situation is complex. One important task is to estimate the nonlinear system performance from the nonlinear characteristics of the devices. In this study, we attempt to establish a connection between them by examining different technologies. Although the orthogonal component has a good correlation with nonlinear system performance, its measurement is prohibitively complex. In the nonlinear noise to power ratio measurement, a certain frequency component of the input signal is notched, and the re-growth component at the notch frequency is measured at the nonlinear device output. The ratio between the re-growth component power and the output signal power is the noise to power ratio. While this method is easy to carry out, it does not correctly estimate nonlinear impairment in general. The reason for this is that the signal incurs different nonlinear responses in two conditions, i.e., with or without a notch. This method accurately estimates the nonlinear impairment in some special but useful cases, such as Gaussian input signals and nonlinear systems whose dominant nonlinear term is the even order term.

Highlights

  • W ITH the increase of network traffic, optical communication uses a higher baud rate and higher modulation order

  • The orthogonal component has a good correlation with nonlinear system performance, but the measurement is difficult

  • In the nonlinear system performance estimation, the equalizer compensates for the IQ imbalance that is included in the linear model but cannot compensate for the IQ imbalance that is included in the equivalent additive noise

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Summary

INTRODUCTION

W ITH the increase of network traffic, optical communication uses a higher baud rate and higher modulation order. In terms of modulation order, 15 GBaud 2048QAM transmission over 100 km was demonstrated in [4], and 130 GBaud dual-polarization probabilistic constellation shaped 256QAM transmission was reported in [5] In such high speed and high order modulation systems, the device imperfections turn out to be significant [6]. The major network traffic occurs in the metro and data-center networks In such application, transmission impairments such as fiber nonlinearity are insignificant, whereas device imperfection turns out to be the primary source of impairment [7]. In [8], we briefly reviewed the linear and nonlinear device imperfection modeling, characterization, and measurement for optical coherent transceivers.

DEVICE LINEAR IMPERFECTIONS
Device Imperfection Measurement in the Laboratory
In-field Measurement before Service
In-field Measurement after Service
Summary of Device Linear Imperfections
Overview of Device Nonlinear Imperfections, Modeling and Specifications
DEVICE NONLINEAR IMPERFECTIONS
Equivalent Additive Noise Model
Total Harmonic Distortion and Nonlinear Terms
Orthogonal Components
Nonlinear Noise to Power Ratio
CONCLUSION
Summary of Device Nonlinear Imperfections
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