FTTx PON Networks: Fiber and Related Issues
Dr. André Girard, Senior Member of Technical Staff
Optical fiber is a key component of the passive optical network (PON), be
it a point-to-point (P2P) or a point-to-multipoint (P2MP) architecture. The
general critical issues related to fiber can be divided into two categories:
- Optical
- Absorption/attenuation
- Chromatic dispersion and polarization mode dispersion (CD and PMD)
- Non-linear effects
- Mechanical
Optical Issues
The fiber of choice for PONs is the singlemode dispersion-unshifted fiber,
based on ITU-T Recommendation G.652 or IEC 60793-2-50 Ed 2. Figure 1
illustrates the typical geometry of this fiber type.
Figure 1. Typical geometry of singlemode dispersion-unshifted fiber
used in a PON
Two types of G.652 fiber are available for PONs, depending on whether or not
the 1383 nm water peak is present. It is important to note that there are
no chromatic dispersion (CD) and polarization mode dispersion (PMD) impairments
for PONs (CD may become an issue only when FP lasers are used at very high
bit rate).
However, non-linear effects (NLEs) can become a problem in PONs using high-power
video signals at 1550 nm. These NLEs are due to changes in the fiber’s
dielectric properties (index of refraction) or stimulated scattering when
using a very high electric field; i.e., the higher the optical power levels
(at constant surface area), the higher the electric field. Nonetheless, when
a certain input intensity is reached, the output intensity will follow a
non-linear curve, thus no longer increasing linearly. This particular input
intensity is called the non-linearity threshold. The field intensity for
a given power level is greater with a smaller fiber core, and longer fiber
lengths decrease the threshold for NLE.
The table below shows how NLEs affect PONs. The most detrimental effect comes
from the Brillouin stimulated scattering, which is due to the very high power
used in overlaid analog video transmission. Digital IP video should dramatically
decrease this effect.
Table 1 – General non-linear effects and how they affect PONs
Phenomenon |
Name |
Nature |
Applicability |
Remarks |
Index of refraction |
SPM |
1λ |
Maybe |
At 1550 nm |
XPM |
Nλ |
|
WWDM |
4WM |
Nλ |
|
WWDM |
Stimulated scattering |
Brillouin |
1λi to 1λj |
Expected |
At 1550 nm
backscattering |
Raman |
1λ to BB |
|
From 1550 to 1600 nm |
SPM = Self-phase modulation
XPM = Cross-phase modulation
4WM = Four-wave mixing
BB = Broadband
Mechanical Issues
As for mechanical aspects, they too can potentially affect the performance
of a PON, The following is a list of common mechanical issues to be aware
of:
- Bending
- macrobending
- microbending
- Discontinuities/gaps/voids
- Misalignments/mismatches
- Cracks/angular or straight breaks
- Dirt in connections
- Fiber melt/fusion splicing
Macrobending (or simply bending) refers to excessive fiber curvature that
causes loss of light (see Figure 2). When the fiber is bent too much, the
angle of total internal reflection between the fiber core and the cladding
is no longer met; and since the angle of total internal reflection is what
ensures the effective propagation of light inside the core, macrobending
can be a major issue as it will reduce the optical energy of the signal.
Longer wavelengths (such as 1625 nm and 1650 nm) are more sensitive to macrobending
than shorter wavelengths are.
Figure 2. Macrobending in optical fiber
Microbending, on the other hand, is a microscopic bend or bump in the fiber
core (shown in Figure 3) and is a possible cause of polarization mode dispersion
(PMD) in optical fiber.
Other causes of disruptions include discontinuities, gaps, voids, misalignments,
mismatches, angular faults, cracks and dirt, and they typically occur during
the connection of two fibers.
Figure 2. Microbending in optical fiber
All of the above cases can affect the signal traveling through an optical
fiber and they mostly occur when human intervention is required (e.g., when
joining a fiber).
In addition, if extremely high optical power is used localized laser heating
may occur and potentially generate a thermal shockwave back to source. At
~1 m/s the wave produce effects balanced between thermal diffusion
and light absorption: thermal lensing caused by the periodic bubbling effect
in the fused region (as shown in Figure 3.29). Local fiber fusion has been
observed at power levels from 0.5 to 3 MW/cm2.
Fiber Cable Types Used in P2MP PONs
There are three types of cable used in the P2MP PON:
(a) Feeder Cable (from the CO
to the splitter distribution hub)
The feeder cable usually has a loose-tube (all-dielectric) design and is the
recommended cable type for most PON applications (armor cable is recommended
if the cable is directly buried). Figure 3.29 illustrates a possible feeder
cable design.
The ANSI/ICEA2 S-87-640-1999, Fiber-Optic Outside Plant Communications
Cable standard defines the requirements for a general-purpose outdoor cable
for both the feeder and the distribution cables.
(b) Distribution Cable (from
the splitter to the drop enclosures)
The distribution cable typically follows the specifications defined for the
feeder cable, even though it supports fewer fibers per cable. The distribution
cable maybe a ribbon fiber type.
(c) Drop Cable (from the drop
enclosures to the premises)
TIA Sub-Committee FO-4.2 Optical Fibers and Cables, has designated
ICEA S-110-717-2003, Optical Drop Cables standard as the drop cable specification
suitable for FTTP (TIA 472F000).
For more on FTTx PON technology, please refer to the FTTx
PON Technology and Testing book or our pocket-sized FTTx
PON Reference Guide. |