Advanced Optical Measurements in Next Generation Networks October 2007 Mike Harrop

Slides:



Advertisements
Similar presentations
Unit-2 Polarization and Dispersion
Advertisements

Some Recent Topics in Physical-Layer System Standards Felix Kapron Standards Engineering Felix Kapron Standards Engineering.
Kazuo Yamane Photonic systems development dept.
S Digital Communication Systems Fiber-optic Communications - Supplementary.
Chromatic Dispersion Measurement methods  Pulse Delay Method (time-of-flight) ‏ IEC / ITU-T G650.1 EIA/TIA-455- FOTP-175-B  Phase Shift Method.
Waveguides Seminary 5. Problem 5.1 Attenuation and crosstalk of a wire pair A carrier frequency connection is transmitted on twisted pairs with the following.
Chapter-3-1CS331- Fakhry Khellah Term 081 Chapter 3 Data and Signals.
TRANSMISSION FUNDAMENTALS Review
Optical Interfaces Lab Last Update Copyright 2014 Kenneth M. Chipps Ph.D. 1.
EE 230: Optical Fiber Communication Lecture 13
EE 230: Optical Fiber Communication Lecture 17 From the movie Warriors of the Net System Considerations.
Fiber-Optic Communications
1 Improving Chromatic Dispersion Tolerance in Long-Haul Fibre Links using Coherent OOFDM M. A. Jarajreh, Z. Ghassemlooy, and W. P. Ng Optical Communications.
EE 230: Optical Fiber Communication Lecture 4
Tutorial on optical fibres F. Reynaud IRCOM Limoges Équipe optique F. Reynaud IRCOM Limoges Équipe optique Cargèse sept 2002.
Polarization Measurements
SKA and Optical Fibre Links R.E. Spencer JBO Dec 2001 Fibre links Fibre optics and link design Array configurations Cost implications.
Module 3.0: Data Transmission
Pitfalls in fibre network design
Lightwave Communications Systems Research at the University of Kansas.
Dispersion Measurements Lecture-3. Dispersion Measurements Measurement of Intermodal Dispersion The most common method for measuring multimode fiber bandwidth.
Reports of optical fiber communication systems
System Performance Stephen Schultz Fiber Optics Fall 2005.
1 Fiber Optic Measurement Technique Piotr Turowicz Poznan Supercomputing and Networking Center Training Session Kiev 9-10 October.
Fiber Bragg Gratings.
Chapter 4 Digital Transmission
L5 Optical Fiber Link and LAN Design
Vadim Winebrand Faculty of Exact Sciences School of Physics and Astronomy Tel-Aviv University Research was performed under a supervision of Prof. Mark.
1 Fiber Optics FIBER PERFORMANCE. 2 Fiber Optics The purity of optical fiber is critical for the best transmission of an optical signal inside a fiber.
Poznan Supercomputing and Networking Center
Review: The application layer. –Network Applications see the network as the abstract provided by the transport layer: Logical full mesh among network end-points.
Optical Fiber Basics-Part 2
Light Wave Systems Dr Manoj Kumar Professor & Head Department of ECE DAVIET,Jalandhar.
Test Plan for PMD Testing of a WDM Receiver Henry Yaffe, Principal January 2004.
SJD/TAB1 EVLA Fiber Selection Critical Design Review December 5, 2001.
May 19, 2011.
Dense Wavelength Division Multiplexing (DWDM) Technology
PROPAGATION OF SIGNALS IN OPTICAL FIBER 9/20/11. Light Characteristics Particle Characteristics Light has energy Photons are the smallest quantity of.
Fotonica in SURFnet6 Wouter Huisman Netwerkdiensten, SURFnet.
May 19-22, 2003 TERENA Networking Conference Zagreb, Croatia1 Optically Amplified Multigigabit Links in CESNET2 network Jan Radil Leoš Boháč Miroslav Karásek.
Intermode Dispersion (MMF)
Chapter 4: Optical fibers and their parameters Graphic representation of three different types of how the refractive index change in the core of an optical.
LOSSES IN FIBER OPTIC SYSTEM
§2 Optical Fibres – a brief introduction Anatomy of a Fiber Cable Fig. 2.1: Anatomy of a fiber.
Chapter 8 Basic System Design. System factors for designing from scratch: Design Verification FactorAvailable choices Type of fiberSingle mode, multimode,
CHAPTER 7 SYSTEM DESIGN. Transmission Types Two types of transmissions: - Link (point to point) - Network -point to multipoint -Mesh -Ring.
PMD Measurement Methods  Fixed Analyzer Method IEC / ITU-T G.650.2/ EIA/TIA Standard FOTP-113  Jones Eigenanalysis Matrix Method IEC /
Investigations on PMD-induced penalties in 40 Gbps optical transmission link Irfan Ullah Department of Information and Communication Engineering Myongji.
The Physical Layer Lowest layer in Network Hierarchy. Physical transmission of data. –Various flavors Copper wire, fiber optic, etc... –Physical limits.
Optical telecommunication networks.  Introduction  Multiplexing  Optical Multiplexing  Components of Optical Mux  Application  Advantages  Shortcomings/Future.
Adaphed from Rappaport’s Chapter 5
Electromagnetic Spectrum
© 2006 EXFO Electro-Optical Engineering Inc. All rights reserved. Agenda Introduction Digital Transmission Dispersion in optical Networks. Dispersion challenges.
Deploying 40Gbps Wavelengths and Beyond  Brian Smith.
Phase velocity. Phase and group velocity Group velocity.
UPM, DIAC. Open Course. March TIME DISPERSION 3.1 Introduction 3.2 Modal Dispersion 3.3 Chromatic Dispersion 3.4 PMD 3.5 Total Dispersion 3.6 Dispersion.
Chromatic Dispersion Compensation for VCSEL Transmission for Applications such as Square Kilometre Array South Africa E K Rotich Kipnoo, H Y S Kourouma,
Kayukov Valeriy Optical System Engineer Step Logic April 15, 2016 Cisco Optical Networking – Chromatic Dispersion calculation. Cisco Support Community.
Sistemas de Comunicación Óptica
A System View of Optical Fiber Communication
Topics discussed in this section:
GROUP DELAY Group delay per unit length can be defined as:
Prof. Manoj Kumar Dept. of Electronics and Communication Engineering
Optical Fiber.
Sandis Spolitis, Inna Kurbatska, Vjaceslavs Bobrovs
The Optical Fiber and Light Wave Propagation
The University of Adelaide, School of Computer Science
A System View of Optical Fiber Communication prt.2
IP over DWDM NANOG May 24, 1999 Larry McAdams
Back End & LO PDR April 2002 FIBRE-OPTIC LINKS -An Introduction Ralph Spencer Jodrell Bank Observatory University of Manchester UK --The use of.
Presentation transcript:

Advanced Optical Measurements in Next Generation Networks October 2007 Mike Harrop

Agenda Introduction Digital Transmission Dispersion in optical Networks. Dispersion challenges for 40G OSA challenges for 40G/ROADM’s

What is the fundamental of digital transmission…? Tx Rx The Rx circuit is clocking at the system line rate and ‘simply’ needs to discern between a 1 and a 0 to recover the original signal.

The need for speed…

Eye diagram at Rx demonstrates signal quality Low BERT Intermediate BERT Unacceptable BERT

BERT causes a lot of pain to transmission groups Typical values for acceptable BERT levels:  >> 1 x  (or 1 bit error per 1,000,000,000,000 bits sent) In terms of QoS measurements:  single BIT error = 1 error second on the network Conclusion of high BERT:  Networks inability to operate at high speed  Poor QoS figures

What’s important in Optical Networks Source : British Telecom Laboratories Technical Journal 2003 (authors Sikora, Zhou and Lord), Advanced network parameters which have to be properly evaluated

What is Dispersion? Dispersion is the time domain spreading or broadening of the transmission signal light pulses - as they travel through the fibre OutRX In TX

Types of Dispersion Chromatic Dispersion: Different wavelengths travel at different velocities Polarization mode dispersion: Different polarization modes travel at different velocities Pulse Pulse Spreading Pulse Pulse Spreading

Types of Dispersion Chromatic Dispersion: Is deterministic Is linear Is not affected by environment Can be compensated Polarization mode dispersion: Is stochastic Is not linear Is affected by the environment Cannot be easily compensated

Chromatic Dispersion October 2007 Mike Harrop

Source wavelengths = do not propagate at the same speed, thus arrive at different times A pulse transmitted in such way suffers a spread, dispersion, limiting the transmission bandwidth. Chromatic Dispersion Issue Pulse Pulse Spreading

Visualizing CD Let’s visualize a light pulse travelling into a fiber and segment it into 9 quadrants (easier to visualize, and to draw!!!)

Visualizing CD Fiber length: Light pulse: Pulse width

Effects of Dispersion

Why is Measuring Dispersion so important? As transmission speeds go up, the residual dispersion allowable at the receiver to give a fixed system penalty goes down. Receiver Tolerance for a 1dB power penalty 2.5 Gb/s16,000ps/nm 10 Gb/s1,000ps/nm 40 Gb/s 60ps/nm e.g. An 80km link at 1550nm will build up 17ps/(nm.km) x 80km = 1360ps/nm. Therefore at data rates at 10Gb/s and higher it is necessary to compensate for the chromatic dispersion. To compensate effectively you need to measure the dispersion of the link.

16 times less CD, cause 1 Time slot 125 us Faster means less time between pulses

The chirp effect Pulse before Gb/s P P P P modulation 16 times less CD, cause 2 Faster means broader pulses

Dispersion Compensation Good News : CD is stable, predictable, and controllable. Dispersion compensating fiber (“DC fiber”) has large negative dispersion -85ps/(nm.km) DC fiber modules correct for chromatic dispersion in the link delay [ps] 0 d TxTx RxRx DC modules fiber span

Dispersion Compensation for DWDM Consider 3 channel SMF system Dispersion (ps/(nm.km)) Wavelength (nm) SMF-28 DCF Slope = 0ps/nm^2/km Dispersion -D +D Distance SMF after 80km 1530nm 1550nm 1570nm Using 16km of 85 ps/(nm.km). Gives a residual dispersion of 1530nm 1550nm 1570nm

Dispersion Compensation for DWDM Dispersion compensation modules can only compensate exactly for one wavelength DWDM system design requires knowledge of end-to-end CD as a function of wavelength… especially for long-haul Dispersion Transmission path 10 Gb/s Tolerance -D +D -D +D 40 Gb/s Tolerance For 40Gb/s transmission slope compensators will be required.

CD: Bad compensation

Dispersion Compensation for DWDM Note. In practise system vendors don’t compensate perfectly for CD at each stage. Usually a system will be pre-compensated and then not brought back to zero during transmission. This is to avoid additional non-linear penalties such as Four Wave Mixing and Cross Phase Modulation. Dispersion Z D Accumulated -D +D D Res +D -D Transmission path

Types of Dispersion Chromatic Dispersion: Different wavelengths travel at different velocities Pulse Pulse Spreading Chromatic Dispersion: Is deterministic Is linear Is not affected by environment Can be compensated

Chromatic Dispersion - Conclusion For 10Gbits/s and higher DWDM systems we need to measure both the dispersion and the slope accurately. Many ways to measure CD in fibre but with the tolerances required for accurate compensation – the only accepted method for making this measurement with this sort of accuracy is the Phase shift method

Measuring Chromatic Dispersion October 2007 Mike Harrop

Patented FTB-5800 method: Source Oscillator DUT or FUT Optical filtering Phasemeter Chromatic dispersion Measurement Method- Phase Shift FOTP-169

Ref Test 1 Few kms of fiber RGD 1

Chromatic dispersion Measurement Method- Phase Shift FOTP-169 Test 2 Few kms of fiber Ref RGD 2

Chromatic dispersion Measurement Method- Phase Shift FOTP-169 Test 3 RGD 3 Few kms of fiber ADVANTAGES: - More points: more resolution - Ideal for compensation - Ideal for complex networks Ref

Reference and Measured Spectral Regions The system compares spectral regions about 1 nm width (A,B,…) with a reference to find the relative group delay and compute CD

Measuring CD Delay points are acquired Lamdba Delay (ps) Lamdba Points are fitted according to models Delay (ps) Slope of Delay gives CD Lamdba CD (ps/nm)

n The by-default or user selected mathematical model is fitted to the RGD point using the generalized least square method. u 3-term Sellmeier (Standard fiber) u 5-term Sellmeier u Lambda Log Lambda u Cubic (Unknown fiber, flattened fiber and amplified links) u Quadratic (Compensating, DSF and NZDSF fibers) u Linear RGD Fitting

Standard Fiber

Extrapolated 0 = nm CD at 1550nm = ps/nm.km Standard Fiber

0 = nm DSF Fiber

Example of NZDSF Analyzed with the help of the FTB-5800 NZDSF fiber (True Wave®)

Specifications Good repeatabilityGood accuracy

EXFO FTB-5800 l Industry leading accuracy on CD and Slope l Ideal for 10G-40G compensation l Source Shape insensitivity l EDFA testing l time saving l Component characterisation l Fast measurement l Powerful but simple software Measuring Chromatic Dispersion

Polarization Mode Dispersion October 2007 Mike Harrop

Reminder Polarization mode dispersion: Different polarization modes travel at different velocities Pulse Pulse Spreading Polarization mode dispersion: Is stochastic Is not linear Is affected by the environment Cannot be easily compensated

Visualizing PMD Let’s visualize a light pulse travelling into a fiber and segment it into 9 quadrants (easier to visualize, and to draw!!!)

Visualizing PMD Fiber section: Light pulse: Pulse width

PMD Impact If we transmit 1-0-1: With PMD, this becomes: The « 1 » is dimmer, the « 0 » can have light: BER

Asymmetries in fiber during fiber manufacturing and/or stress distribution during cabling, installation and/or servicing create fiber local birefringence. A "real" long fiber is a randomly distributed addition of these local birefringent portions. What causes PMD

What causes PMD? Fiber defects Environmental constraints GeometricInternal Stress Lateral Pressure Bend Heat Wind (aerial fibers)

Small Birefringence

Fast Slow

Large Birefringence

Fast Slow

Birefringence and mode coupling

Fast Slow

Causes of PMD Birefringence (Bad)  Introduced during manufacture  non uniform intrinsic fibre stresses ie core concentricity  non uniform extrinsic stresses ie pressure Mode coupling (Good)  fibre bend and twist  in-built stress in “spun” fibre  splices

PMD - Lower Bit Rate fast axis z, t slow axis  t T0T0 T

PMD - Higher Bit Rate fast axis z, t slow axis  t

PMD vs Wavelength and Time Pradeep Kumar Kondamuri and Christopher Allen Information and Telecommunications Technology Center, The University of Kansas, Lawrence, Kansas, Douglas L. Richards Sprint Corporation, Overland Park, Kansas

1dB Penalty probability: Very low Average PMD System Tolerance Low PMD average

1dB Penalty probability: low Average PMD System Tolerance Limit PMD average

1dB Penalty probability: very high Average PMD System Tolerance Too high PMD average

A PMD outage is when the instantaneous DGD exceeds a given threshold (Max DGD) A factor 3 between Max DGD and Average PMD is taken from a number of ITU ‑ T Recommendations (including G OPTICAL TRANSPORT NETWORK PHYSICAL LAYER INTERFACES ) for % of no PMD problems Once you know the system tolerance (Max DGD), aim at PMD < 1/3 of this value if you transmt Sonet/SDH PMD Power Penalty

PMD Pass-Fail criteria ITU-T G.959.1, version 7.6 defines Max DGD as 3* It also defines Max DGD as 30ps for OC-192 ITU-T G.650 places it at 25ps Max DGD, but this is based of FIBER, with no allowance to components. Good for Fiber Manufacturer, too tight for NSP IEEE-802.3ae has Max DGD at 19ps (10 GigE), and with a tolerance of % (Corporation, Banks, etc need higher security) Max DGD is divided by 3.73 for this level

PMD vs Outage probability System vendors give Max DGD. You choose Outage probabliity, then calculate PMD to achieve

Maximum PMD value to ensure % probability that the tolerable broadening will correspond to a mean power penalty of 1 dB. SONET-SDH Bit rate (Gbit/s) Average PMD* (ps) Digital Transmissions PMD Specifications

Maximum PMD value to ensure % probability that the tolerable broadening will correspond to a mean power penalty of 1 dB 10 GigE Bit rate (Gbit/s) 10 Average PMD* (ps) 5 Digital Transmissions PMD Specifications

Total PMD vs PMD Coefficient Total link PMD (ps) 10ps over 400km 5ps over 50km Which is better? PMD Coefficient (ps/√km) used by fibre & cable manufacturers, based on ITU recommendations that a network will be 400km. For 10G Total limit is 10ps, using our network length of 400km gives: 10ps √400km = 0.5ps/ √km

Typical values for new fibre. G.652 Standard Single Mode <0.1ps/  km G.655 NZDSF <0.04ps/  km e.g. For a 80km SMF link you would expect to see 0.1 x sqrt(80km) = 1ps Delay For a 80km NZDSF link you would expect to see 0.04 x sqrt(80km) = 0.36ps Delay Installed base?

Installed Base Source: John Peters, Ariel Dori, and Felix Kapron, Bellcore 10G 40G

Reminder Polarization mode dispersion: Different polarization modes travel at different velocities Pulse Pulse Spreading Polarization mode dispersion: Is stochastic Is not linear Is affected by the environment Cannot be easily compensated

Pitfalls Chromatic Dispersion: Should be specified at the cable specs (install or rental of dark fiber) Should be tested/compensated on installation or ahead of system turn up Should be considered very deeply for DWDM systems Polarization mode dispersion: Should be specified at the cable spec level (install or rental of dark fiber) Fibers should be tested and classified for suitability of different lines speeds High levels could mean very costly re-engineering

Conclusions Uncontrolled fiber dispersion leads to increased BERT and lower QoS metrics Dispersion should be considered mission critical to any operator considering high speed digital transmission Accurate measurement and interpretation of those data are critical…

Measuring Polarization Mode Dispersion October 2007 Mike Harrop

TIA/EIA FOTP 124 : Polarisation Mode Dispersion for Single-mode fibres by Interferometry. Traditional Interferometric Method (TINTY) Limitations Gaussian Interferogram Smooth ripple free, Gaussian like source Ideal random coupling DUT Autocorrelation Peak Cross correlation Half width Gaussian fit Broadband Source Polarizer FUT Interferometer Mirror Analyzer Detector

FOTP-124: Are these Gaussian??? Saudi Arabia: South Africa:

FOTP-124: Are these Gaussian??? USA: UK:

FOTP-124: Are these Gaussian??? UK:

? Source Shape Auto-correlation Infinitely broad sourceInfinitely thin line Broad uniformVery thin peak Odd-looking spectrum Broad peak, humps, ripple, etc… Add Autocorrelation to Crosscorrelation Autocorrelation: source shape

TIA/EIA FOTP 124a : Polarisation Mode Dispersion for Single-mode fibres by Interferometry. Generalised Interferometic Method (GINTY) No Limitations No reliance on Gaussian Interferogram Any fibre or component can be measured Any source shape acceptable Broadband Source Polarizer Interferometer Mirror Analyzer PBS Detectors FUT

FOTP PMD Calculation for Fibers with Strong Mode Coupling The PMD delay,, is determined from the half width parameter,  , of the Gaussian curve fitting applied to the interferogram according to: Where   is the RMS width of the Gaussian calculated from the interferogram … 6.2 Accuracy Accuracy is related to the capability to precisly fit the interferogram with the Gaussian function …

What do the standards say? Ref. IEC Fibre Optic communication system design guides – Part 9: Guidance on PMD measurements and theory

Measuring PMD FTB-5500B: l Highest accuracy and resolution l Ideal for 10G-40G compliance & certification l Source Shape insensitivity l Test the whole link l EDFA, OADM testing l Fast measurement time l Powerful but simple software l Same source as FTB-5800 CD Analyzer

Polarization Optical Time Domain Reflectometer October 2007 Mike Harrop

What to do with a link with high PMD? Frequent PMD problems (not measured when built) Need a way to find high PMD sections: PMD TOT =  N (PMD N ) 2 Example: 15ps, 2ps, 1ps, 6ps 225ps 2 + 4ps 2 + 1ps ps 2 = 266ps /2 = 16.31ps Find the 15ps section, replace it, problem solved…

Birefringence & Mode Coupling fast slow h fast slow fast slow fast slow Fibres with short (h) where Fast & Slow axis change frequently, tend to have low PMD Fibres with long (h) where Fast & Slow axis Change infrequently, tend to have high PMD

DOP Polarization-OTDR Quantitative  =  not measured  PMD value not measured DOP SOP1, DOP SOP2, h and L = all measured  Tendency for High PMD fiber under test Pulsed DFB Laser Detector Polarimeter /4 Polarizer /4 SOP 1 /SOP 2 4x2 OTDR acquisitions for characterizing SOP(z)

Example of Measurement and Validation (1) Link Length ~ 41 km PMD = 9.8 ps PMD coefficient ~ 3 ps/  km Cable opened and PMD measured with EXFO FTB-5500B PMD test set: 29 km, PMD = 4.3 ps 5 km, PMD = 17.4 ps 7 km, PMD = 6.9 ps 29 km 5 km 7 km High Contrast

Example of Measurement and Validation (2) Link Length ~ 41 km PMD = 9.8 ps PMD coefficient ~ 1.53 ps/  km Cable opened and PMD measured with EXFO FTB-5500B PMD test set: 6 km, PMD = 9.25 ps 35 km 6 km High Contrast

Bi-directional Measurements Quite similar results

Fiber Mapping in a Cable km Fiber # PMD (ps) Open and test Source: Connibear, A.B. and Leitch, A.W.R., Uni. Port Elizabeth, “Locating High PMD Sections of an Overhead Cable Unsing Polarization OTDR” Fiber # PMD (ps) km Replace and retest fiber#

Questions?