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IK2211_OptNetwModule_2010 (1)

Course: ICT 3, Spring 2011
School: Kungliga Tekniska...
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Data IK2211 Links and LANs Optical Networks module Lena Wosinska wosinska@kth.se The Royal Institute of Technology (KTH), School of Information and Communication Technology (ICT) Next Generation Optical NETworks (NEGONET) http://www.ict.kth.se/MAP/FMI/Negonet/ Outline Introduction Development of optical networks Telecom market evolution Overview of broadband access technologies Evolution of fiber access...

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Data IK2211 Links and LANs Optical Networks module Lena Wosinska wosinska@kth.se The Royal Institute of Technology (KTH), School of Information and Communication Technology (ICT) Next Generation Optical NETworks (NEGONET) http://www.ict.kth.se/MAP/FMI/Negonet/ Outline Introduction Development of optical networks Telecom market evolution Overview of broadband access technologies Evolution of fiber access networks Passive Optical Network (PON) Current generation PON Next generation PON: short term and long term development PON protection schemes Reliability performance vs. cost tradeoff in PON. Conclusions Lena Wosinska 2 Development of optical networks What Is An Optical Network? It is NOT NECESSARILY all optical packet switched Characteristics of an optical network Transmission: optical Switching: could be optical, could be electronic, could be hybrid could be circuit, could be packet, could be burst First-generation optical networks Transmission in the optical domain (to provide capacity) Example: SONET network (Synchronous Optical Network) More functionality in the optical domain (optical networking) Second-generation optical networks Circuit Switched Optical Networks (wavelength routed networks) Some of routing, switching and intelligence is moving into the optical layer Third-generation optical networks (?) 3 Lena Wosinska Internet Model Most widely used WAN technology IP: the network protocol that is designed to operate above a variety of data link layer (network access) protocols Lena Wosinska 4 Multiple protocol stacks ATM network SONET network IP router ATM switch SONET cross-connect Lena Wosinska IP router 5 Photonics in switching Optical circuit switching (OCS) Wavelength-routed networks Relatively mature technology today Providing lightpaths A lightpath corresponds to a circuit Set-up a lightpath The whole lightpath is available during the connection Disconnect WDM network elements: OLT, OADM, OXC Not available today due to some technological problems Optical packet switching (OPS) Controllable optical memory for optical buffering, control functions in the optical domain, synchronization, etc Optical burst switching (OBS) Hybrid packet switching: a feasible solution? Lena Wosinska 6 Optical Networking (OCS) Circuit switched optical networks Lightpath Optical connection Transparent Routed One wavelength channel on each link Wavelength conversion Spans multiple links Transparency Lena Wosinska 7 The optical layer The optical layer provides lightpath service to its client layers. Lightpath: optical connection An optical channel trail between two nodes that carries the entire traffic within a wavelength Lena Wosinska 8 Functions of the optical layer Multiplexing wavelengths Switching and routing wavelengths Monitoring network performance at various locations in the network Client layers of the optical layer: SONET/SDH ATM (Asynchronous Transfer Mode) IP Lena Wosinska 9 WDM Core Network OLT OXC Lightpath OADM IP IP Lena Wosinska 10 Traffic demand drivers User behavior Always on (reachability, upgrades and downloads) File sharing Services High-Speed Internet VoIP IPTV Gaming Telemedicine E-Goverment etc Triple play Traffic increases very rapidly 11 Lena Wosinska Triple play capacity requirements 3P Telephony Basic 3P and extended 3P Number of channels Capacity 1 80 kb/s symmetric Basic 3P 2 TV Extended 3P Internet access Basic 3P 1 10 Mb/s symmetric 30 Mb/s symmetric Extended 3P 4 2 x 9 Mb/s 4 x 15 Mb/s asymmetric asymmetric Basic: design for basic triple play today Extended: design for five years from now 12 Lena Wosinska Development in Sweden COMPUTER AT HOME Population INTERNET AT HOME BROADBAND AT HOME Year 13 Broadband access technologies Telecom Network Hierarchy Long haul - 100s-1000s km - Mesh Metro (interoffice) - 10s of km - Rings Access - a few km - Hubbed rings, PONs Users The Last Mile First 15 Lena Wosinska Broadband access technologies Digital subscriber loop DSL (from telcos) High-speed digital access to the Internet Based on existing twisted pair Cable (from cable TV companies) Wireless access: WIMAX, WIFI, 3G Fiber access Fiber to the cabinet (FTTCab) Fiber to the curb (FTTC) or Fiber to the Building (FTTB) Fiber to the home(FTTH) Lena Wosinska 16 Broadband access technologies: limitations Access based on: Capacity/user ADSL VDSL Coax Wi-Fi WiMax EPON GPON 2 Mb/s (typical) 20 Mb/s (typical) 2 Mb/s * 54 Mb/s (max) 28 Mb/s (max) 60 Mb/s * 40 Mb/s * Max Reach 5.5 km 1 km 0.5 km 0.1 km 15 km 20 km 20 km FTTx * Bandwidth depends on the number of users Lena Wosinska 17 OECD broadband statistics Source: OECD Other are mostly fixed wireless access (3G or WIMAX) In Japan and Korea the DSL penetration decreases because of swap to FTTH FTTx completely dominated by a few national operators in Japan and Korea China not an OECD member and therefore not included here 18 Lena Wosinska www.oecd.org/sti/ict/broadband FTTH growth prediction Forecasts for Europe (subscribers in thousands) IDATE predicts a drop in active ADSL in Europe from 2010 (in Japan happened in 2006) In 2016 FTTX users are estimated to grow to 30% of the total broadband lines. (Ref: IDATE February 2007) Lena Wosinska 19 Evolution of fiber access networks Fiber To The X (FTTx) Why fiber access? Internet ONT Leased Line Frame/Cell relay ONU OLT NT Telephone Interactive Video ONU ODN Copper ODN Copper ODN Fiber is a future proof infrastructure FTTH/O Low attenuation long distances High capacity many broadband users FTTB/C But Too expensive to roll out overnight Other access technologies will complement FTTCab (especially wireless) In some areas FTTH is not economically viable CO Electronics OLT ONT ONU NT Lena Wosinska Optical line terminal Optical network termination Optical network unit Network termination NT Home network NIU 21 Point-to-Point links Simple, standardized and mature technology N Users CO L km Lena Wosinska 22 Active Optical Network Simple, standardized and mature technology N subscribers Curb Switch CO L km Lena Wosinska 23 Passive Optical Network (PON) Simple, under standardization technology Passive devices (splitters). No active elements in the signals path from source to destination Passive Optical Splitter L km N subscribers CO Lena Wosinska 24 Comparison P2P links N fiber lines 2N transceivers Concentration switch in the neighborhood 1 fiber line Power in the field 2N + 2 transceivers PON 1 fiber line N + 1 transceivers Path transparency Lena Wosinska 25 Wireless fiber and common platform Core network Wimax, FWA C/DWDM links Radio over Fibre with C/DWDM links Hot spot, WLAN FTTC+VDSL FTTH Mobile 3G/4G Lena Wosinska 26 Passive Optical Networks PONs and reliability models Basic PON topologies Ring topology Tree topology Bus topology Lena Wosinska 28 Passive architectures Advantages Simple Easy to operate Do not have any active devices in the outside plant Do not need to be powered Time Division Multiplex PON (TDM PON) PON architectures Ethernet PON (EPON) Gigabit PON (GPON) A broadcast-and-selected WDM PON (WPON) A wavelength-routing PON (WRPON) Lena Wosinska 29 Time vs. Spectrum Sharing TDM-PONs: Current generation PON Standardized Use few wavelengths (typically 2 or 3) Low cost and mature devices (splitters, lasers, etc.) Limited power budget Maximum distances 20km, Split ratios 64 Traffic distribution Broadcast scheme downstream TDMA techniques upstream Examples: APON/BPON, EPON & GPON WDM-PONs: Next generation PON (long term) Proposed in literature and/or demonstrated Introduce WDM technology and devices (AWG) Long-reach and high bandwidth Examples: CPON, LARNET, RITENET, Success-DWA Hybrid WDM/TDM-PONs: Next generation PON (short term) Lena Wosinska 30 TDM PON Downstream traffic is broadcasted to all ONUs Low security ONUs filter data (frames) by destination address Upstream traffic is time division multiplexed at the RN Upstream and downstream traffic is sent at different wavelengths to share one fiber between OLT and RN Lena Wosinska 31 PON with analogue video overlay Data and voice in both directions Video in only one direction Video on dedicated wavelength all the way to ONU Analogue video overlay commonly used in the US in FTTx installations (temporary solution) Lena Wosinska 32 Ethernet PON (EPON) EPON preserves 802.3 frame format EPON uses existing MAC EPON uses existing 8B/10B encoding EPON uses standard 802.3 line rate (1 Gbps) 320 million Ethernet ports deployed worldwide (~95% of all switch ports) Focus: simplicity and integrity of Ethernet Work is done by IEEE802.3ah task force Lena Wosinska 33 Downstream Transmission passive optical splitter Downstream channel is broadcast. 802.3 Frames extracted by ONUs. Lena Wosinska 34 Upstream Transmission Upstream time slicing No packet fragmentation No collisions How to schedule ONUs?: static vs. dynamic bandwidth allocation Lena Wosinska 35 WDM PON WRPON: Wavelength Routed PONs (incl. AWG) WPON: WDM broadcast and select PONs Lena Wosinska 36 Hybrid WDM/TDM-PON Lena Wosinska 37 PON protection schemes and reliability models Motivation Evolution of broadband access networks towards FTTH. Passive optical networks (PONs): an attractive option. Growing importance of reliable access to (broadband) network services. Access network is very cost sensitive minimizing the cost for network protection Lena Wosinska 39 Main issue: low cost solutions Requirements on technology Core Low installation and operational cost i.e. low CAPEX and OPEX Metro Access Requirements on cost effectiveness Lena Wosinska 40 Protection schemes Standard protection schemes (ITU-T G.983.5 ) Type A: feeder fiber (FF) is duplicated Type B: FF and optical interface at OLT are duplicated Type C: 1+1 path protection all resources duplicated Type D: full/partial protection Novel (cost efficient) protection schemes for hybrid WDM/ TDM PON Investment cost for burying redundant DFs to each optical network unit can be saved CAPEX reduction Efficient utilization of wavelength reduction of number of wavelengths needed for protection Lena Wosinska 41 Standard schemes (ITU-T G.983.5 ) Lena Wosinska 42 Novel Protection Scheme 1 Hybrid WDM/TDM PON J. Chen and L. Wosinska, Analysis of protection schemes in PON compatible with smooth migration from TDM-PON to hybrid WDM/ TDM-PON, OSA Journal of Optical Networking, Vol. 6, No 5 (May 2007) Built-in redundancy where two neighbouring ONUs protect each other Main advantages: (i) no extra DFs are needed for protection CAPEX saving (ii) protection for both FF and DF failures is provided. (iii)1:1 link protection provides good reliability performance Our approach minimizes the investment cost for protection while keeping connection availability at the acceptable level Lena Wosinska 43 Novel Protection Scheme 1 Lena Wosinska 44 Novel Protection Scheme 2 Hybrid WDM/TDM PON Jiajia Chen, L. Wosinska, and S. He, High Utilization of Wavelengths and Simple Interconnection Between Users in a Protection Scheme for Passive Optical Networks, IEEE Photonics Technology Letters, Vol. 20, No 6, pp: 389 391 (March15, 2008) Utilizing the cyclic property of the AWG our protection scheme has three main advantages (compared to the existing schemes): (i) 50% fewer wavelengths are needed; (ii) in the case of DF break there is no influence on the remaining ONUs; (iii) protection for FF failure is provided. Our approach maximizes the wavelength utilization for protection while maintains an acceptable level of connection availability Lena Wosinska 45 Novel Protection Scheme 2 Normal operation Lena Wosinska 46 Novel Protection Scheme 2 Protection In the case of distributed fiber-cut between AWG and ONU1,1 In the case of feeder fiber-cut between OLT and AWG Lena Wosinska 47 Ring Protection (1) Normal operation Protected operation Lena Wosinska 48 Ring Protection (2) SUCCESS-HPON Lena Wosinska 49 Conclusions Broadband access (at least 10 Mb/s in short run) to every household Next-generation access network will be based on fiber PON is considered to become the choice TDM PON (EPON and GPON): today 10GPON and Hybrid WDM/TDM PON: short term (D)WDM PON: long term Next-generation access network must be reliable and robust Protection CAPEX and OPEX need to be very low Scalability Lena Wosinska 50 Topics for this module and reliability models Fiber access network architectures Point-to-point (P2P) Active optical network (AON) Passive optical network (PON) Definitions Scalability Cost Performance (power budget, security, etc) Passive Optical Networks PON topologies Resource sharing in PON (TDM vs. WDM) TDM PON, WDM PON, hybrid WDM/TDM PON Current and next generation PON Performance parameters Long Reach PON TDM Passive Optical Networks Review standards Compare physical layers and MAC layers Compare performance Define conditions where GPON is better than EPON and vice versa. Motivate. Bandwidth allocation Static bandwidth allocation (SBA) Semi-static Bandwidth allocation (S-SBA) Dynamic bandwidth allocation (DBA) Lena Wosinska 55
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GWU - PHYS - 2163
Waves, the Wave Equation, and Phase VelocityWhat is a wave? Forward [f(x-vt)] and backward [f(x+vt)] propagating waves The one-dimensional wave equation Harmonic waves Wavelength, frequency, period, etc. 0 1 2 3f(x) f(x-2) f(x-1) f(x-3)xPhase velocity
GWU - PHYS - 2163
What is a wave?A wave is anything that moves. To displace any function f(x) to the right, just change its argument from x to x-a, where a is a positive number. If we let a = v t, where v is positive and t is time, then the displacement will increase with
GWU - PHYS - 2163
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GWU - PHYS - 2163
Proof that f (x vt) solves the wave equationu = 1 and Write f (x vt) as f (u), where u = x vt. So xNow, use the chain rule:f f = x uf f u = x u x f f u = t u t2 2 f 2 f =v 2 t u 2u =v tSo2 f 2 f x 2 = u 2andf f =v t u Substituting into the wave
GWU - PHYS - 2163
The 1D wave equation for light waves2 E 2 E 2 = 0 2 x tWell use cosine- and sine-wave solutions: where E is the light electric fieldE ( x, t ) = B cos[k ( x vt )] + C sin[k ( x vt )]orkx (kv)tE ( x, t ) = B cos(kx t ) + C sin(kx t )where: k=v=1
GWU - PHYS - 2163
A simpler equation for a harmonic wave:E(x,t) = A cos[(kx t) ]Use the trigonometric identity:cos(zy) = cos(z) cos(y) + sin(z) sin(y)where z = k x t and y = to obtain:E(x,t) = A cos(kx t) cos( ) + A sin(kx t) sin( )which is the same result as before,
GWU - PHYS - 2163
Definitions: Amplitude and Absolute phaseE(x,t) = A cos[(k x t ) ]A = Amplitude = Absolute phase (or initial phase)
GWU - PHYS - 2163
DefinitionsSpatial quantities:Temporal quantities:
GWU - PHYS - 2163
DefinitionsSpatial quantities:Temporal quantities:
GWU - PHYS - 2163
Human waveA typical human wave has a phase velocity of about 20 seats per second.
GWU - PHYS - 2163
The Phase of a WaveThe phase is everything inside the cosine.E(x,t) = A cos( ), where = k x t = (x,y,z,t) and is not a constant, like !In terms of the phase, = / t k = / xAnd / t v = This formula is useful when the wave is really complicated. / x
GWU - PHYS - 2163
Complex numbersConsider a point, P = (x,y), on a 2D Cartesian grid.Let the x-coordinate be the real part and the y-coordinate the imaginary part of a complex number. So, instead of using an ordered pair, (x,y), we write: P = x+iy = A cos( ) + i A sin( )
GWU - PHYS - 2163
Euler's Formulaexp(i ) = cos( ) + i sin( )so the point, P = A cos( ) + i A sin( ), can be written:P = A exp(i )whereA = Amplitude = Phase
GWU - PHYS - 2163
Proof of Euler's Formula exp(i ) = cos( ) + i sin( )Use Taylor Series:x x2 x3 f ( x) = f (0) + f '(0) + f '(0) + f '(0) + . 1! 2! 3!x x 2 x3 x 4 exp( x) = 1 + + + + + . 1! 2! 3! 4! x 2 x 4 x 6 x8 cos( x) = 1 + + + . 2! 4! 6! 8! x x3 x5 x 7 x9 sin( x) =
GWU - PHYS - 2163
Complex number theoremsIf exp(i ) = cos( ) + i sin( )exp(i ) = 1 exp(i / 2) = i exp(-i ) = cos( ) i sin( ) 1 cos( ) = [ exp(i ) + exp(i )] 2 1 sin( ) = [ exp(i ) exp(i ) ] 2i A1exp(i1 ) A2 exp(i 2 ) = A1 A2 exp [ i (1 + 2 ) ]A1exp(i1 ) / A2 exp(i 2 ) =
GWU - PHYS - 2163
More complex number theoremsAny complex number, z, can be written: So and z = Recfw_ z + i Imcfw_ z Recfw_ z = 1/2 ( z + z* ) Imcfw_ z = 1/2i ( z z* )where z* is the complex conjugate of z ( i i ) The "magnitude," | z |, of a complex number is: | z
GWU - PHYS - 2163
We can also differentiate exp(ikx) as if the argument were real.d exp(ikx) = ik exp(ikx) dx Proof : d [ cos(kx) + i sin(kx)] = k sin(kx) + ik cos(kx) dx 1 = ik sin( kx) + cos(kx) i But 1 / i = i, so : = ik [ i sin(kx) + cos(kx) ]
GWU - PHYS - 2163
Waves using complex numbersThe electric field of a light wave can be written:E(x,t) = A cos(kx t )Since exp(i ) = cos( ) + i sin( ), E(x,t) can also be written:E(x,t) = Re cfw_ A exp[i(kx t )] orE(x,t) = 1/2 A exp[i(kx t )] + c.c.We often write the
GWU - PHYS - 2163
Waves using complex amplitudesWe can let the amplitude be complex:E ( x, t ) = A exp i ( kx t ) E ( x, t ) = cfw_ A exp(i ) exp i ( kx t ) cfw_where we've separated the constant stuff from the rapidly changing stuff.The resulting "complex amplitude
GWU - PHYS - 2163
Waves using complex amplitudesWe can let the amplitude be complex:E ( x, t ) = A exp i ( kx t ) E ( x, t ) = cfw_ A exp(i ) exp i ( kx t ) cfw_where we've separated the constant stuff from the rapidly changing stuff.The resulting "complex amplitude
GWU - PHYS - 2163
The 3D wave equation for the electric field and its solution!A light wave can propagate in any direction in space. So we must allow the space derivative to be 3D: orr2 2 E E 2 = 0 t2 E 2 E 2 E 2 E + 2 + 2 2 = 0 2 x y z twhich has the solution: where a
GWU - PHYS - 2163
rr E0 exp[i (k r t )] is called a plane wave. %A plane waves contours of maximum field, called wave-fronts or phase-fronts, are planes. They extend over all space.Wave-fronts are helpful for drawing pictures of interfering waves.A wave's wavefronts swe
GWU - PHYS - 2163
Laser beams vs. Plane wavesA plane wave has flat wave-fronts throughout all space. It also has infinite energy. It doesnt exist in reality. A laser beam is more localized. We can approximate a laser beam as a plane wave vs. z times a Gaussian in x and y:
GWU - PHYS - 2163
exp(-x2)Laser pulsesx If we can localize the beam in space by multiplying by a Gaussian in x and y, we can also localize it in time by multiplying by a Gaussian in time.Et t2 x2 + y 2 E ( x, y, z , t ) = E0 exp 2 exp exp[i (kz t )] 2 % % w This is t
GWU - PHYS - 2163
Longitudinal vs. Transverse wavesMotion is along the direction of propagation longitudinal polarizationLongitudinal:Transverse:Motion is transverse to the direction of propagation transverse polarizationSpace has 3 dimensions, of which 2 are transver
GWU - PHYS - 2163
Vector fieldsLight is a 3D vector field.rr A 3D vector field f (r )assigns a 3D vector (i.e., an arrow having both direction and length) to each point in 3D space.Wind patterns: 2D vector fieldA light wave has both electric and magnetic 3D vector fie
GWU - PHYS - 2163
The 3D wave equation for the electric field is actually a vector equation!A light-wave electric field can point in any direction in space:r r2 r E E 2 = 0 t2Note the arrow over the E.which has the solution: where and andr r k ( k x , k y , k z ) r (
GWU - PHYS - 2163
Waves using complex vector amplitudesWe must now allow the complex field E and its amplitude E0 to be % % vectors:rr rr r E ( r , t ) = E0 exp i k r t % %()Note the arrows over the Es!The complex vector amplitude has six numbers that must be specifi
GWU - PHYS - 2163
Light is not only a wave, but also a particle.Photographs taken in dimmer light look grainier.Very very dim Very dim DimBrightVery brightVery very brightWhen we detect very weak light, we find that its made up of particles. We call them photons.
GWU - PHYS - 2163
PhotonsThe energy of a single photon is: h or h = (h/2 )where h is Planck's constant, 6.626 x 10-34 Joule-sec. One photon of visible light contains about 10-19 Joules, not much!. is the photon flux, or the number of photons/sec in a beam. = P / h where
GWU - PHYS - 2163
Counting photons tells us a lot about the light source. Random (incoherent) light sources,such as stars and light bulbs, emit photons with random arrival times and a Bose-Einstein distribution. Laser (coherent) light sources, on the other hand, have a mo
GWU - PHYS - 2163
Photons have momentumIf an atom emits a photon, it recoils in the opposite direction.If the atoms are excited and then emit light, the atomic beam spreads much more than if the atoms are not excited and do not emit.
GWU - PHYS - 2163
PhotonsRadiation PressurePhotons have no mass and always travel at the speed of light. The momentum of a single photon is: h/ , or hk Radiation pressure = Energy Density (Force/Area = Energy/Volume)When radiation pressure cannot be neglected: Comet tail
GWU - PHYS - 2163
Photons"What is known of [photons] comes from observing the results of their being created or annihilated."Eugene HechtWhat is known of nearly everything comes from observing the results of photons being created or annihilated.
GWU - PHYS - 2163
Maxwell's Equations and Light WavesVector derivatives: Div, grad, curl, etc. Derivation of wave equation from Maxwell's Equations Why light waves are transverse waves Why we neglect the magnetic field
GWU - PHYS - 2163
Div, Grad, Curl, and all thatTypes of 3D vector derivatives:The Del operator:r , , x y z The Gradient of a scalar function f :r f f f f , , x y z If you want to know more about vector calculus, read this book!The gradient points in the direction of
GWU - PHYS - 2163
Div, Grad, Curl, and all thatThe Divergence of a vector function:rr f x f y f z f + + x y zThe Divergence is nonzero if there are sources or sinks.A 2D source with a large divergence:y xNote that the x-component of this function changes rapidly in t
GWU - PHYS - 2163
Div, Grad, Curl, and more all thatTheLaplacianofascalarfunction: rr r f 2f ff f = , , x y z =2 f 2 f 2 f + + 2 2 x y z 2TheLaplacian of a vectorfunctionisthesame, butforeachcomponentoff:r 2 fx 2 fx 2 fx 2 f y 2 f y 2 f y 2 fz 2 fz 2 fz 2 f = 2 + +
GWU - PHYS - 2163
Div, Grad, Curl, and still more all thatr The Curl of a vector function f :rr f z f y f x f z f y f x f , , y dz z dx x dy The curl can be treated as a matrix determinant :x r r f = x fx y y fy z z fz Functions that tend to curl around have large
GWU - PHYS - 2163
A function with a large curlr f ( x, y, z ) = ( y, x, 0) r f (1, 0, 0) = (0,1, 0) r f (0,1, 0) = (1, 0, 0) r f (1, 0, 0) = (0, 1, 0) r f (0, 1, 0) = (1, 0, 0)yxr r f z f y f y f x f x f z f = , , y z z x x y = ( 0 0, 0 0, 1 (1) ) =( 0, 0 , 2)$ So th