Optical Switching

Chapter 3.3 - Enabling Technologies For Optical Packet Switching

3.3   ENABLING TECHNOLOGIES FOR OPTICAL
PACKET SWITCHING


The technologies presented in this section are of critical importance for the realization
of practical and cost-effective all-optical OPS nodes. Most of these technologies
are also considered vital for optical packet switches with electronic control
but with transparent handling of optical data.

3.3.1   All-Optical 3R Regeneration

In order for an optical signal that remains in optical form throughout its journey in
the optical cloud to be successfully received on the other side, its power levels and
quality must fall within specified limits. Optical signals are susceptible to various
impairments caused by attenuation, noise, dispersion, crosstalk, jitter, and nonlinear
effects. The effects of these impairments accumulate as the signal travels in the
network and are exacerbated as the transmission span, number of wavelength channels
per fiber, and bit rate per channel increase. Unfortunate consequences include
significant amplitude loss, pulse shape distortion, and timing drifts [14].

The losses in amplitude could be compensated by optical amplifiers. However,
these devices do not correct distorted pulse shapes and they amplify both the
signal and the noise, thereby leading to further degradations in signal quality. In
other words, the signal needs to be cleaned up before it is amplified. The process
of recovering the original signal shape and removing impairments is referred to as
3R regeneration as it includes reamplification, reshaping, and retiming of the
signal as well. The pulse shaping problem is reduced by dispersion compensation,
which counterbalances the spread in pulse width caused by chromatic dispersion.
Retiming is accomplished by clock extraction and synchronization (packet-level
synchronization for synchronous networks and bit-level synchronization for asynchronous
networks). To retime the signal, data rate and format have to be known
to the regenerator and the latter must be capable of bit rate flexible operation
[14]. 3R regeneration may be required at several points in the network depending
on its diameter and the number and type of devices that signals traverse.

The most widely used approach for 3R regeneration requires conversion of the
signal to the electrical field. This is because optical implementation of some regeneration
functions, such as retiming, is challenging with the current technology.
All-optical 3R regeneration, however, is regarded as an important technology to
enable, and simplify, OPS implementation.

Attempts to realize all-optical 3R regeneration are currently limited to experimentation.
A 3R unit is composed of three main blocks: an amplifier, a clock recovery
system, and a threshold detection unit. The clock is extracted from the amplified
signal. It is then combined with the signal to produce time-realigned pulses. The
regenerated signal appears at the output of the threshold detector [14].

Most of optical 3R regeneration efforts are based on semiconductor optical
amplifier based Mach–Zehnder interferometers (MZIs). They offer high speed
and low switching energy, and their fabrication techniques are mature enough to
obtain almost polarization-insensitive operation. Another method uses the concept
of soliton transmission combined with in-line synchronous intensity/phase modulation
and optical narrowband filtering. Because of the separation of reshaping
and retiming, this method has the potential for simultaneous regeneration of
several WDM channels. The clock recovery system must be capable of very fast
locking to incoming optical signals and production of flexible repetition rates.
Despite laboratory demonstrations, all-optical 3R regeneration is still in the
experimental phase and is not available today for commercial deployment [14].

 

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