Unitary Matrices in Fiber Optical Communications: Applications

Similar documents
Low-complexity Algorithms for MIMO Multiplexing Systems

, on the power of the transmitter P t fed to it, and on the distance R between the antenna and the observation point as. r r t

Chapter 7. Interference

Computer Propagation Analysis Tools

MIMO Cognitive Radio Capacity in. Flat Fading Channel. Mohan Premkumar, Muthappa Perumal Chitra. 1. Introduction

Lecture 22 Electromagnetic Waves

The Production of Polarization

Lecture 17: Kinetics of Phase Growth in a Two-component System:

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

The k-filtering Applied to Wave Electric and Magnetic Field Measurements from Cluster

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch. Rui Li, J. Bisognano, R. Legg, and R. Bosch

On Control Problem Described by Infinite System of First-Order Differential Equations

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

PAPER On the Capacity of MIMO Wireless Channels

Range Migration Techniques for Short-Range MIMO Array Imaging

Reinforcement learning

Variance and Covariance Processes

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

The shortest path between two truths in the real domain passes through the complex domain. J. Hadamard

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

Statistical/Evolutionary Models of Power-laws in Plasmas

On Energy-Efficient Node Deployment in Wireless Sesnor Networks

Monochromatic Wave over One and Two Bars

Short-hops vs. Long-hops - Energy efficiency analysis in Wireless Sensor Networks.

The sudden release of a large amount of energy E into a background fluid of density

Transmit Beamforming with Reduced Channel State Information in MIMO-OFDM Wireless Systems

Revision of Lecture Eight

The Global Trade and Environment Model: GTEM

[ ] 0. = (2) = a q dimensional vector of observable instrumental variables that are in the information set m constituents of u

CS 188: Artificial Intelligence Fall Probabilistic Models

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2

ENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]

Chapter Finite Difference Method for Ordinary Differential Equations

Pressure Vessels Thin and Thick-Walled Stress Analysis

On The Estimation of Two Missing Values in Randomized Complete Block Designs

7 Wave Equation in Higher Dimensions

Turbo-Like Beamforming Based on Tabu


Extremal problems for t-partite and t-colorable hypergraphs

Representing Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example

Stress Analysis of Infinite Plate with Elliptical Hole

Feedback Couplings in Chemical Reactions

FINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement

A Study on Non-Binary Turbo Codes

APPLICATION OF MAC IN THE FREQUENCY DOMAIN

Fullwave Analysis of Thickness and Conductivity Effects in Coupled Multilayered Hybrid and Monolithic Circuits

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f

MECHANICS OF MATERIALS Poisson s Ratio

Chapter 3: Theory of Modular Arithmetic 38

Kalman Filter: an instance of Bayes Filter. Kalman Filter: an instance of Bayes Filter. Kalman Filter. Linear dynamics with Gaussian noise

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

Quantum Algorithms for Matrix Products over Semirings

Orthotropic Materials

Measures the linear dependence or the correlation between r t and r t-p. (summarizes serial dependence)

A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS

Pseudosteady-State Flow Relations for a Radial System from Department of Petroleum Engineering Course Notes (1997)

r r r r r EE334 Electromagnetic Theory I Todd Kaiser

Today - Lecture 13. Today s lecture continue with rotations, torque, Note that chapters 11, 12, 13 all involve rotations

The Great Wave Hokusai. LO: Recognize physical principles associated with terms in sonar equation.

control properties under both Gaussian and burst noise conditions. In the ~isappointing in comparison with convolutional code systems designed

PHYS PRACTICE EXAM 2

Massive MIMO Systems with Non-Ideal Hardware: Energy Efficiency, Estimation, and Capacity Limits

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

Envelope and Phase Distribution of Two Correlated Gaussian Variables

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

r P + '% 2 r v(r) End pressures P 1 (high) and P 2 (low) P 1 , which must be independent of z, so # dz dz = P 2 " P 1 = " #P L L,

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 121 FINAL EXAM

Electromagnetism Physics 15b

The evolution of the phase space density of particle beams in external fields

Risk tolerance and optimal portfolio choice

On Capacity-Maximizing Angular Densities of Multipath in MIMO Channels

Sharif University of Technology - CEDRA By: Professor Ali Meghdari

Research & Reviews: Journal of of Statistics and Mathematical Sciences

AST1100 Lecture Notes

EE3723 : Digital Communications

Ferent equation of the Universe

(a) Unde zeo-bias conditions, thee ae no lled states on one side of the junction which ae at the same enegy as the empty allowed states on the othe si

Vehicle Arrival Models : Headway

PROBLEM SET #1 SOLUTIONS by Robert A. DiStasio Jr.

Goodness-of-fit for composite hypotheses.

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Exponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.

HW Solutions # MIT - Prof. Please study example 12.5 "from the earth to the moon". 2GmA v esc

arxiv: v1 [math.co] 4 Apr 2019

Circular Motion. Radians. One revolution is equivalent to which is also equivalent to 2π radians. Therefore we can.

OPTIMIZATION OF TOW-PLACED, TAILORED COMPOSITE LAMINATES

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

Mixture Regression-Cum-Ratio Estimator Using Multi-Auxiliary Variables and Attributes in Single-Phase Sampling

you of a spring. The potential energy for a spring is given by the parabola U( x)

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Transcription:

Uniay Maices in Fibe Opical Communicaions: Applicaions Ais Mousaas A. Kaadimiais Ahens P. Vivo KCL R. Couille Pais-Cenal L. Sanguinei Pisa A. Mulle Huawei H. Hafemann Huawei Ais Mousaas, Univesiy of Ahens

Inoducion eed fo high speed infasucue Bandwidh BW hungy echnologies emeging ~2 db incease pe yea -Wied: IPTV, elepesence, online gaming, live seaming ec. - Capaciy- cunch eminen Soluions so fa Opical ewos WDM-DWDM have exploied many degees of feedom BW, available powe, polaizaion divesiy excep one: spaial. Soon he online devices will exceed he numbe of global populaion! Use of opical Space Division Muliplexing SDM is compelling. Ideally: wihou changing he aleady infasucue Ais Mousaas, Univesiy of Ahens 2

Inoducion Wha is Opical MIMO? Jus lie in wieless domain, in opical we can use paallel ansmission pahs o gealy enhance he capaciy of he sysem. Fis pape on Opical MIMO: H. R. Sua, Dispesive muliplexing in mulimode opical fibe, Science 2895477, 28 283 2 Muli-Mode Fibes MMF: Use muliple modes o cay infomaion Muli-Coe Fibes MCF: Uilize diffeen opical pahs of diffeen coes in he same fibe wihin he same cladding Ais Mousaas, Univesiy of Ahens 3

Inoducion Poblem: Cossal phenomenon aises Cossaling beween adjacen coes in MCF Ligh beam scaeing esuling in cossaling in MMF Due o : Exensive fibe lengh Bending of fibe Limied aea wih muliple powe disibuions Ligh beam scaeing on-lineaiies Ais Mousaas, Univesiy of Ahens 4

Inoducion Poblem: Cossal phenomenon Two Appoaches: Figh i Secion of 7-coe opical fibe Ais Mousaas, Univesiy of Ahens 5

Inoducion Poblem: Cossal phenomenon Two Appoaches: Tae advanage of i Classic MIMO echniques equied bu wih some wiss: Low powe consains o avoid non-linea behavio. Opical channel maix jus a subse of a uniay maix. Ais Mousaas, Univesiy of Ahens 6

Sysem Model Conside a single-segmen -channel lossless opical fibe sysem: ansmiing channels excied, eceiving channels coheenly. The 2 2 scaeing maix is S T SS T Only Haa-disibued I sub-maix is of inees is ~. Geneally, < : Ohe channels may be used fom diffeen, paallel ansceives Modelling of loss: addiional enegy los duing popagaion Ais Mousaas, Univesiy of Ahens 7

Sysem Model Only Haa-disibued I sub-maix is of inees is ~.......... Define x maix U as T U P SP whee P pojecion opeao: P I - Ais Mousaas, Univesiy of Ahens 8

Sysem Model Channel Equaion: Assume no diffeenial delays beween channels fequency fla fadinghe muual infomaion is I y Ux I U U log U log de λ z Gaussian noise z Receive nows he channel pilo Tansmie does no now he channel w.l.o.g. Ais Mousaas, Univesiy of Ahens 9

Ais Mousaas, Univesiy of Ahens Infomaion Meics Ouage Pobabiliy: Opimal: Assumes infinie codewods Wha is he pice of finie codelenghs? Gallage eo bound fo M-lengh code: [ ] Pob U U ou I E I P Θ < < U U I U log de max exp M E P e

Coulomb Gas Analogy Join pobabiliy disibuion of eigenvalues of UU U λ λ,..., λ exp log λ log λ 2 log λ P, 2 Ν λm 2 Exponen is enegy of poin chages epelling logaihmically in he pesence of exenal field 2 S [ p] P e Lage : chages coalesce o densiy Dyson Ben Aous/Maida S dx p x Veff x dxdy p y p xlog x y Veff x n log x β log x whee n β Minimizing convex S w.. px gives he Maceno-Pasu disibuion p MP x x a b x 2πx x a, b n ± β n β n β 2 > m Ais Mousaas, Univesiy of Ahens

Ouage Pobabiliy We need ails of disibuion: Opical Comms opeae a P ou I < E [ Θ I ] Pob U U p ou 8 Fouie ansfom o use lage deviaions agumens S S V eff x V eff dx p x x log log x x plays ole of sengh of logaihmic aacion/epulsion a x > shifs chage densiy o lage values R>Reg, < o smalle ones R<Reg Minimizing S w.. px gives he genealized Maceno Pasu disibuion Equivalen o balancing foces on he chage locaed a x: p x' n β 2P dx x x' x x Ais Mousaas, Univesiy of Ahens 2

Genealized MP equaion Use Ticomi heoem o calculae px Obain closed fom exp. fo enegy S[p] E.g. β>; n> p x b x x a 2πx x n x a b β x ab a, b, calculaed fom p b p a b x dxp xlog a b dxp x a Ais Mousaas, Univesiy of Ahens 3

Genealized MP equaion In geneal S b S ab S S a a b< a> b< a b a> b n; β < c -- c < < c2 > c2 n>; β < c3 > c3 -- -- n; β> -- < c4 -- > c4 n>; β> -- all -- -- Phase ansiions a o a> ec ae hid ode disconinuous S' '' Relaion o Tacy-Widom? c Ais Mousaas, Univesiy of Ahens 4

Ais Mousaas, Univesiy of Ahens 5 Disibuion Densiy of Finally whee is he vaiance a he pea of he disibuion. [ ] eg S S v e f eg 2π 2 2 4 log '' b a a b S v eg eg

umeical Simulaions β > and n > The LD appoach demonsaes bee behavio, following Mone Calo. Ais Mousaas, Univesiy of Ahens 6

umeical Simulaions β > and n > The LD appoach demonsaes bee behavio, following Mone Calo. Fo small values of, and, he discepancy is minimal Ais Mousaas, Univesiy of Ahens 7

Ais Mousaas, Univesiy of Ahens 8 Finie Bloc-Lengh Eo Pobabiliy Hee we need whee ow is bounded in [,] Also when < ohewise no consain x x V x V x x p dx S S eff eff log log α α < j j e M E P λ log max exp U x x x x dxp b a log Ν Μ α

umeical Simulaions β > and n Thee ae wo ypes of phase ansiion poins hee: c : A poin disconinuous S' ' c2 : Disconinuous S' '' c2 c 2 8 6 Eo Pobabiliy vs Rae; P; β3; n α2 α α5 op 4 2 -logpe/ 2 8 6 4 2.5.5 2 2.5 Ais Mousaas, Univesiy of Ahens 9

Moe Realisic Channel Chaoic caviy picue: S I 2πiW π H i WW W Assuming vey low bacscaeing a edges we obain U P SP cp H G iγ P Deeminisic mode enegy Random complex Gaussian Diagonal loss maix Γ H G Ais Mousaas, Univesiy of Ahens 2

Ais Mousaas, Univesiy of Ahens 2 Moe Realisic Channel Muual Infomaion meic: I Disibuion mean-vaiance can be obained using eplica heoy I 2 same wih also expessions fo vaiance [ ] i i I P Γ G H P P Γ G H P I G log de [ ] [ ] 2 2 2 log de p p I I I I E δ H G 2 2 2 p T p p T p p T δ δ δ δ H H H H

umeical Simulaions Ais Mousaas, Univesiy of Ahens 22

Conclusions MIMO: pomising idea in Opical Communicaions In his wo: Simple model fo Opical MIMO channel Lage Deviaion Appoach povides ails fo MIMO muual infomaion Mehod povides meic fo ouage houghpu and finie bloclengh eo Many issues sill open: Channel modeling sill a is infancy Tansmie/Receive Achiecues Muliple fibe segmens onlineaiies Ais Mousaas, Univesiy of Ahens 23

Inoducion Moivaion: Cap cunch, degees of feedom Channel Model: Uniay, andom, lossyefeence fo exa channel model on-lineaiies, MDL Meics: Capaciy Equaion, dof explanaion Eo exponen: Poof by Gallaghe Eigenvalue picue: Mapping o effecive enegy minimize o maximize pobabiliy: MP esul fo mos pobable Coulomb appoach: effecive densiy Inegal equaion and soluion Examples of mos pobable densiies compaison beween opimal and nonopimal ouage Ais Mousaas, Univesiy of Ahens 24

Inoducion Phase ansiions: Second ode and hid ode ansiions in he Gallaghe exponens Genealizaion o ohe appoaches Deeminisic plus andom channel Lossy channel Amplify and fowad channel Ais Mousaas, Univesiy of Ahens 25