Title: Rollout SURFnet6 progress report
1Roll-out SURFnet6 progress report
May 17th, 2005
Roeland Nuijts Network Services
Department SURFnet BV roeland.nuijts_at_surfnet.nl
2Outline
- Introduction
- SURFnet6 WDM network
- Dark fiber requirements testing
- Loss
- Optical reflections
- Dispersion
- PMD
- Experiences
- System tests of SURFnet6
- Timeline SURFnet6 build progress
3Dark fibers in SURFnet6
- five DWDM subnetworks for transporting the IP
traffic and lightpaths and connecting the various
add/drop sites in SURFnet6 - all transmission fiber is leased DFs (Dark
Fibers), mix of standard SMF (G.652) and NZ-DSF
(G.655) - 40 DF pairs for DWDM
- 37 DF pairs for TDM
- 8 suppliers
- one CfP
- one subnetwork finished (subnetwork 3) and
tested, four under construction - OADM sites for adding and dropping
wavelengths/lightpaths - DWDM system
- maximum 72 wavelengths _at_ 10Gb/s, total capacity
of 720Gb/s per subnetwork - modular design for adding wavelengths
4Requirements for Dark Fibers
- Loss lt 0.25dB/km (_at_ 1550nm)
- splice loss lt 0.15 dB, max no. splices 1 per
2km - connector loss lt 0.5 dB, generally accepted but
properly treated connector should easily meet
0.2dB - Optical reflections below -30dB
- Fiber type G.655 (preferred) or G.652
- PMD lt 0.5 ps/?km
- SC-PC (flat) connectorized
- practical, easy to use
- sufficient performance if well treated
5Loss
- Fiber loss is wavelength dependent, minimum is
around 1550nm - Current fiber loss is close to fundamental limit
which arises from Rayleigh scattering (scattering
caused by local variations in density and
therefore refractive index), proportional to ?-4
therefore dominant at short wavelengths - Loss at long wavelengths (? gt 1625nm) dominated
by infra-red absorption - Peak at 1400nm arises from OH impurities, can be
removed (AllWave fiber)
6Reflections
- Main source of reflections, mismatch in
refractive index
n1
n2
Pinc
Ptrans
Preflc
Example reflection of a glass-air interface is
about 2.8 which corresponds to -15.5dB
7Reflections
- Sources of reflections, mismatch in refractive
index - Airgaps in connections
- Offset in alignment
- Bad or dirty connections
- Glas-air interface (end of fiber)
- MPI (Multi Path Interference)
- Optical receiver receives desired signal plus
undesired delayed copies of signal, deteriorates
BER (Bit Error Rate) - Acceptable reflection for transmission equipment
is -27dB - Specification for maximum reflection in fibers is
-30dB
fiber1
fiber2
ncladding
ncore
ncladding
ncladding
ncore
ncladding
8Measurement of loss and reflections- OTDRs
(Optical Time Domain Reflectometer)
pre-spool (1km)
post-spool (1km)
OTDR
fiber under test
pulse source
Glass-air interface 15.5dB ? easy sanity check
of OTDR equipment!!
photo detector
digital signal processing
9OTDR- example of measured data
- Trade of between resolution and distance
- Length of pulse 1 ?s x 2.998 108 m/s /1.5 200m
- Short pulse 10 ns ? 2m ? small enough to check
patches in remote central office
10Fiber dispersion G.655 versus G.652
- Refractive index varies with wavelength which
leads to a wavelength dependence of the group
delay, ?g, (delay for different wavelengths) in
ps - Dispersion coefficient, D, is the derivative of
the group delay, ?g , with respect to wavelength
per unit length (ps/nm km)
?g (ps)
? (nm)
Optical signal at Tx output in time domain
D (ps/nm km)
0
? (nm)
?0
?T
- No distortion at zero-dispersion wavelength, ?0
- Distortion at other wavelengths
Optical signal in frequency domain
11Historical perspective
- Early fibers extremely lossy 1000dB/km (1960)
- Progress in fabrication lead to low loss fibers
(0.2dB/km at 1550nm wavelength, limited by
fundamental limit of Rayleigh scattering) around
1979 - Initial (80s) devices for transmission through
single mode fiber operated in the 1310nm
wavelength region, 1550nm devices did not exist - Installed fiber base largely comprised of
standard (1.3µm zero-dispersion wavelength) SMF
(Single Mode Fiber) - This embedded base represents an enormous
investment, strong incentive to use it - Development of commercially available 1550nm
sources and detectors started in 80s - Invention of EDFAs (Erbium Doped Fiber
Amplifiers) for amplification of optical signals
in 80s
12Dispersion limited distance, LD
- Chromatic dispersion places a limit on the
maximum transmission distance - LD scales with square of the bitrate
B 10 Gb/s D 17 ps/nm km LD 50km ??
0.112 nm
- 800km at 2.5Gb/s
- 50km at 10Gb/s, dispersion compensation is
needed in case of transmission beyond 50km
3dB bandwidth of 7GHz assumed, doublesided
spectrum ? 14GHz ? 0.112nm
13Example of impact of dispersion on transmission
systemperformance - optical pulse shape of
10Gb/s signal after 120km
120km standard SMF D17.8 ps/nm km
Tx
Rx
OA
OA
rb 10Gb/s ?c 1557nm
120km-10Gb/s system configuration
Optical pulse shape at transmitter output
- Pulse shape after 120km transmission completely
distorted due to pulse broadening, error-free
transmission not possible
After 120km transmission
14Dispersion Compensating Fiber
Dispersion compensating fiber
Standard fiber
D (ps/nm km)
0
?0, SMF
?T
?0, DCF
? (nm)
- Advantages
- Wide band compensation (one DCF compensates for
all channels in C-band) - Feasible for DWDM systems
- Easy to use, reliable
- Disadvantages
- bulky
- DCF loss, requires additional optical amplifier
- smaller core area, hence nonlinear effects
15Optical pulse shape after 120km and after
DCF(Dispersion Compensating Fiber)
Optical pulse shape at transmitter output
- Pulse shape after 120km transmission completely
distorted due to pulse broadening, error-free
transmission not possible - Optical pulse shape recovered after passing
through DCF with negative dispersion - More residual dispersion if optical power level
at the input of the DCF is high due to the
(undesirable) nonlinear effect in the DCF
After 120km transmission
After compensation
16NZ-DSF (Non-Zero Dispersion ShiftedFiber)
- DSF (zero-dispersion at 1550nm), good for single
channel transmission but causes FWM (Four Wave
Mixing) - NZDSF, finite dispersion in 1550nm DWDM window to
avoid FWM, dispersion slope needs to be
compensated
17PMD (Polarization Mode Dispersion)
- Orthogonal polarizations propagate at different
speeds through fiber which leads to signal
distortion and limits the achievable transmission
distance - More prominent at higher speeds 10Gb/s
- More prominent in old fibers (non-cylindrical
core) - PMD coefficient is given in ps/?km
- PMD coefficient measured by interferometric
method
- Example PMD coefficient 0.5 ps/?km, maximum
differential - delay, ?PMD, is 10 of bit period. In case of
10Gb/s this is 10ps. - Maximum transmission distance is 10ps/(0.5
ps/?km) 20?km - maximum transmission distance 400km
18Measured DF data for DWDM spans
19Summary of experiences with DFs
- Deviation in delivered lengths prompted
re-simulation of dispersion compensation of all
subnetworks - Measurement crews unaware of proper specs
- High reflections unnoticed
- High connector losses unnoticed
- One of reasons is outsourcing
- Traditional telcos deliver worst DF service
- PMD passed (PMD coefficient lt 0.5 ps/?km) in all
but one span - G.653 (DSF, Dispersion Shifted Fiber), supplier
did not notice
20SURFnet6 Subnetwork 3
OSNR (0.1nm) gt 40dB
- Subnetwork 3 specific
- eight spans
- total distance 528km
- dispersion optimized to allow traffic between
any pair of sites
OSNR (0.1nm) gt 28dB
21Test results
- Long term BER-test error-free for 1 day 25 min,
corresponds to BERlt1.1 10-15 - Power supply interruption, no traffic hits
- Simulation of fiber cut, surviving traffic
remained error-free
22Simple formula for OSNR calculation
repeater
SMF
SMF
SMF
DCF
DCF
Tx
Rx
NF2
NF3
NFN-1
NFN
NF1
Pin,1
Pin,2
Pin,3
Pin,N-1
Pin,N
OSNR
Simple formula, accurate to a few tenth of dBs
23General timelines and planning
- September 2004 blueprint version 1.0 finalized
- November 2004 - June 2005 installation by
Telindus - Ring 3 has been completed
- H2 2005 transition connected organizations to
SURFnet6
24Thanks!roeland.nuijts_at_surfnet.nl