Optical Switching

Chapter 3.3.6 - All-Optical Wavelength Conversion

3.3.6   All-Optical Wavelength Conversion

All-optical wavelength conversion is identified as an integral technology in the
effort to implement efficient optical packet switches. The role of wavelength conversion
and its impact on the performance of an optical packet switch is discussed in
Section 3.5. In this section, we present the issues surrounding the technical
implementation of all-optical conversion.

Wavelength converters may be required at the input and/or output interfaces of
an OPS node, or they may be part of buffering systems, all-optical 3R regenerators,
or optical header detectors. Although wavelength conversion can potentially be
implemented via OEO conversions, all-optical wavelength conversion is desirable
in order to maintain the advantages of end-to-end data transparency.

In all-optical wavelength conversion, the optical signal remains in the optical
domain throughout the conversion process [22]. Approaches under research
include wavelength conversion using wave-mixing and cross-modulation in
SOAs. Wave mixing arises from a nonlinear optical response of a medium when
more than one wave is present. It results in the generation of another wave whose
intensity is proportional to the product of the interacting wave intensities. Wave-
mixing preserves phase and amplitude information, offering strict transparency.
It also allows simultaneous conversion of a set of multiple input wavelengths to
another set of multiple output wavelengths and could potentially accommodate
signals with bit rates exceeding 100 Gb/s. The wave-mixing phenomenon that
can be exploited for wavelength conversion is four-wave mixing (FWM), which
the result of the interaction between three optical waves generating a fourth wave
of another frequency. When FWM occurs in an active medium such as a semi-
conductor optical amplifier, it can provide wavelength conversion. This technique
provides modulation-format independence and high bit-rate capabilities. The conversion
efficiency from pump energy to signal energy of this technique, however,
is not very high, and it decreases swiftly with increasing conversion span (shift
between pump and output signal wavelengths) [23, 24].

Wavelength conversion based on cross-modulation utilizes active semiconductor
optical devices such as amplifiers or lasers. One option is to use an SOA in cross-gain
modulation (XGM). In this approach, an intensity-modulated input signal modulates
the gain in the SOA due to gain saturation. A continuous wave signal at the desired
output wavelength is modulated by the gain variation so that it carries the same information
as the original input signal. Although the XGM scheme is simple to realize,
it suffers from inversion of the converted bit stream and extinction ratio degradation
for an input signal up-converted to a signal of equal or longer wavelength [23].

Another approach involves SOAs in cross-phase modulation (XPM). The operation
of a wavelength converter using SOA in cross-phase modulation (XPM)
mode is based on the fact that the refractive index of the SOA is dependent on
the carrier density in its active region. An incoming signal that depletes the
carrier density will modulate the refractive index and thereby result in phase modulation
of a continuous wave signal (wavelength) coupled into the converter. With the
XPM scheme, the converted output signal can be either inverted or noninverted,
unlike in the XGM scheme where the output is always inverted. The XPM
scheme is also very power-efficient compared to the XGM scheme [23].

According to their signal properties, wavelength converters (WCs) can be divided
into three categories [25]:

  1. Variable-input/fixed-output WCs, which can convert several input wavelengths
    into a certain output wavelength.
  2. Fixed-input/variable-output WCs, which can change a certain input
    wavelength into more than one output wavelength, which are often closely
    neighboring the input wavelength.
  3. Variable-input/variable-output WCs, which are capable of converting a band
    of wavelengths into another waveband.

Converters belonging to the third category are referred to as tunable wavelength
converters (TWCs) or tunable optical wavelength converters (TOWCs). Tunable
converters are further divided into two subgroups according to their wavelength conversion
range. Full-range TOWCs are capable of converting any input wavelength
to any of the output wavelengths used on a fiber link. On the other hand, limited-range
wavelength converters can only convert a subset of the available input wavelengths
to a restricted number of output wavelengths [25]. The assumption of limited
wavelength conversion is more realistic given the current technology.

An ideal wavelength converter should have the following characteristics [23]:

  • transparency to bit rates and signal formats;
  • fast setup time;
  • large wavelength span and capability to convert to both shorter and longer
    wavelengths;
  • moderate input power requirements;
  • possibility for same input and output wavelengths (i.e., no conversion);
  • insensitivity to input signal polarization; and
  • minimal distortion of the output signal, that is, high extinction ratio and large
    signal-to-noise ratio. These features determine the cascadeability of wavelength
    converters.

Although considerable progress has been made in all-optical wavelength conversion,
a number of technical issues remain of considerable concern and continue
to represent topics of research. Reliability and cost of all-optical wavelength conversion
are also of concern [14]. None of the existing techniques exhibits all the
desired properties listed above [15].

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