an EDFA site. An alternative scheme involves the use
of the compensating fiber within the cable itself after
having been jointed with the transmission fiber as part
of the overall fiber link. Such DCFs are referred as
reverse/inverse dispersion fibers (RDF/IDF) [60–62].
Reverse dispersion fibers are used with the transmission
fiber almost in the ratio of 1:1, meaning their character-
istic dispersion parameters D and S are almost the same
as that of the trans mission fiber except for the signs.
Thus, for the reverse dispersion fiber used in [60], D
and S were 16 ps/nm$km and 0.050 ps/nm
2
$km,
respectively. Dispersion ramped fiber links, which in-
volve use of RDFs, alternate fiber segments with the
link and consist of positive and negative dispersion
fibers, so that the overall dispersion is low, and D versus
length curve mimicks a sawtooth curve. One major at-
tribute of these fibers was that loss in such fibers was
low (in contrast to high negative D DCFs), ~ 0.25
dB/km. Terabit transmission experimen ts through a re-
peater span of over 125 km were reported in such
dispersion managed fiber links in volving RDFs in con-
junction with G.652 fibers over a bandwidth of 50 nm
[63]. Alternate fiber segments in these links consist of
positive and negative D (in 1:1 ratio) fibers such that
overall dispersion is low and D versus length curve
mimicks a sawtooth curve. RDFs were also used with
NZ-DSFs (in a ratio of 1:2) [64].
3.1.4 Fibers for metro networks
In recent years, metro optical networks have attracted
a great deal of attention from lightwave communication
engineers due to potentials for high growth. A metro
network provides generalized telecommunication ser-
vices trans porting any kind of signal from point to point in
a metro. First-generation metropolitan optical networks
based on SDH/SONETrelied on rings laced with nodes at
which information is electronically exchanged. Access
that aggregates a wide variety of traffic from business and
residential end users is required to port this traffic directly
to the transport product for distribution throughout an
optical network. In transport, DWDM is the key enabli ng
technology to expand the capacity of existing and
new fiber cables without optical-to-electric al-to-optical
Table 3.1.5 Important performance parameters of the designed DSCFs for 6.655 fibers (After [58]; copyright Optical Society of America).
Designed dual-core
DSCF for
D
(ps/nm km)
RDS
(nm
L1
)
A
eff
(mm
2
)
Mode field
diameter (mm)
FOM
(ps/nm dB)
Bend loss *
(dB)
LEAF
Ô
(C-band) 264 0.033 41.8 3.34 1248 2.54 1.0e–02
LEAF
Ô
(L-band) 172 0.017 43.63 3.47 885 4.28 1.0e–03
True Wave RS
Ô
(C-band) 173 0.0099 49.92 3.68 760 2.35 1.0e–06
True Wave RS
Ô
(L-band) 173 0.0075 61.4 4.02 851 1.89 1.0e–06
TeraLight
Ô
(S-band) 201 0.01 45.97 3.42 844 5.2 1.0e–02
TeraLight
Ô
(C-band) 187 0.0084 49.99 3.55 873 6.51 1.0e–03
TeraLight
Ô
(L-band) 150 0.006 57.77 3.92 771 1.4 1.0e–02
Values correspond to central l in each band as in Table 1.4.
*
For a single-turn bend of diameter 32 mm.
0.2
0.1
0
0.1
0.2
0.3
1.53
(a)
Wavelength (μm)
1.54 1.55 1.56
D
ave
(ps/nm.km)
DCF for
LEAF
TM
DCF for
Teralight
TM
DCF for
TrueWave-RS
TM
DCF for
LEAF
TM
DCF for
Teralight
TM
DCF for
TrueWave-RS
TM
Wavelength (μm)
(b)
0.2
0
0.2
0.4
1.57 1.58 1.59 1.6 1.61
D
ave
(ps/nm.km)
Fig. 3.1.26 (a) Net residual dispersion spectra at the C-band of
standard NZ-DSF fiber links jointed with designed dual-core
DSCFs. (b) Net residual dispersion spectra at the L-band of
standard NZ-DSF fiber links jointed with designed dual-core
DSCFs.
104
SECTION THREE Optical Fibers
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