Dense Wavelength Division Multiplexing - DSpace at CUSAT ...
Dense Wavelength Division Multiplexing - DSpace at CUSAT ...
Dense Wavelength Division Multiplexing - DSpace at CUSAT ...
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<strong>Dense</strong> <strong>Wavelength</strong> <strong>Division</strong> <strong>Multiplexing</strong><br />
be transmitted per second. Traditionally, this has been the industry method of choice (DS-1, DS-<br />
2, DS-3 etc.). However, when service providers use this approach exclusively, they must make<br />
the leap to the higher bit r<strong>at</strong>e in one jump, having purchased more capacity than they initially<br />
need. Based on the SONET hierarchy, the next incremental step from 10 Gbps TDM is 40 Gbps<br />
– a quantum leap th<strong>at</strong> many believe will not be possible for TDM technology in the near future.<br />
This method has also been used with transport networks th<strong>at</strong> are based on either the synchronous<br />
optical network (SONET) standard for North America or the synchronous digital network (SDH)<br />
standard for intern<strong>at</strong>ional networks.<br />
Options for Increasing Carrier Bandwidth<br />
Faced with the challenge of dram<strong>at</strong>ically increasing capacity while constraining costs, carriers<br />
have two options: Install new fiber or increase the effective bandwidth of existing fiber.<br />
Laying new fiber is the traditional means used by carriers to expand their networks. Deploying<br />
new fiber, however, is a costly proposition. It is estim<strong>at</strong>ed <strong>at</strong> about $70,000 per mile, most of<br />
which is the cost of permits and construction r<strong>at</strong>her than the fiber itself. Laying new fiber may<br />
make sense only when it is desirable to expand the embedded base. Increasing the effective<br />
capacity of existing fiber can be accomplished in two ways:<br />
• Increase the bit r<strong>at</strong>e of existing systems.<br />
• Increase the number of wavelengths on a fiber.<br />
Increase the Bit R<strong>at</strong>e<br />
Using TDM, d<strong>at</strong>a is now routinely transmitted <strong>at</strong> 2.5 Gbps (OC-48) and, increasingly, <strong>at</strong> 10 Gbps<br />
(OC-192); recent advances have resulted in speeds of 40 Gbps (OC-768). The electronic circuitry<br />
th<strong>at</strong> makes this possible, however, is complex and costly, both to purchase and to maintain. In<br />
addition, there are significant technical issues th<strong>at</strong> may restrict the applicability of this approach.<br />
Transmission <strong>at</strong> OC-192 over single-mode (SM) fiber, for example, is 16 times more affected by<br />
chrom<strong>at</strong>ic dispersion than the next lower aggreg<strong>at</strong>e speed, OC-48.<br />
The gre<strong>at</strong>er transmission power required by the higher bit r<strong>at</strong>es also introduces nonlinear effects<br />
th<strong>at</strong> can affect waveform quality. Finally, polariz<strong>at</strong>ion mode dispersion, another effect th<strong>at</strong> limits<br />
the distance a light pulse can travel without degrad<strong>at</strong>ion, is also an issue.<br />
<strong>Division</strong> Of Computer Engineering, SOE 8