Changing Topology and Communication Delays

Size: px
Start display at page:

Download "Changing Topology and Communication Delays"

Transcription

1 Prepared by F.L. Lews Updated: Saturday, February 3, 00 Changng Topology and Communcaton Delays Changng Topology The graph connectvty or topology may change over tme. Let G { G, G,, G M } wth M fnte be the set of all dgraphs defned for a gven set of nodes V. Let the Laplacan for graph G be denoted L. We tae the case where the graph topology swtches between graphs n ths set. The frst result taes the case where all the graphs G are connected. Lemma [Saber and Murray 004]. Let the swtched control law be ut ( ) Lt ( ) xt ( ) where the correspondng graphs Gt ( ) are each strongly connected and balanced. Then the closed-loop system converges asymptotcally to the average consensus soluton x. Moreover, V x x T T L L T s a common Lyapunov functon. (Proof- V ( xx) ( xx) ( Ls ) xx.) Normally, however, each graph G s not connected. Then, we must tal about how the graphs are related to each other over tme ntervals. The unon of any group of dgraphs contaned n G s a dgraph wth nodes V and edge set gven by the unon of the edge sets of that group. A group of graphs n s sad to be jontly (strongly) connected f ther unon s (strongly) connected [Jadbabae, Ln, Morse 003]. Consder a sequence of dgraphs (V,E(t)) wth t N. A node v s connected to a dstnct node vl V \{ v} acro an nterval I N f v s connected to v l n the dgraph V, E( t) ti [Moreau 005]. A row stochastc matrx M s stochastcally ndecomposable and aperodc (SIA) (or T ergodc) f lm M w wth w a vector. That s, the lmt has ran of one. Lemma. Let M be a non-negatve row stochastc matrx wth a smple e-val at z=. Then all T other e-vals are strctly nsde the unt crcle. Then M s SIA. Furthermore, lm M w where w s the normalzed left e-vector of,.e. wm T w T, w T. Fnally every element of w s nonnegatve.

2 Recall that M s a non-negatve row stochastc matrx wth a smple e-val at z= ff ts graph contans a spannng tree, and f the graph s strongly connected. The next case consders products of matrces, each one of whch may not be SIA. Lemma (Wolfowtz). Let { M, M,, M m } be a fnte set of SIA matrces wth the property that every fnte product of the M s also SIA. Then for each nfnte sequence of matrces M one has lm T M M M w Note that n ths theorem the set of matrces must be fnte. Lemma (Ren and Beard). Let { M, M,, M m } be a set of row stochastc matrces. If the unon of the drected graphs of these matrces contans a spannng tree, then the product M M M s SIA. m Dscrete-Tme Swtchng Models From [Jadbabae, Ln, Morse 003]. They consder UNDIRECTED graphs. Let x( t) x( t) u( t) and ut () ( I Dt ()) Ltxt () (), wth the average headng error gven by et ( ) Lt ( ) xt ( ). (.e. u(t) s the gradent-based control.) Then the closed-loop system s the Vcse [995] system x( t) x( t) xj( t) n ( t) jn () t where n () t N () t. Then the global state dynamcs s x t I D t I A t x t F t x t ( ) ( ()) ( ()) () () () where each F(t) s a stochastc matrx. Lemma. The system acheves consensus f and only f lm FtFt ( ) ( ) F() F(0) w T for some vector w. Frst the easy case. t Lemma. [Jadbabae, Ln, Morse 003]. Let every graph n the swtchng set be connected. Then lm x( t) x, where x s a number dependng only on x(0) and the swtchng sgnal. t

3 Note t s not obvous n the swtched topology case how x depends on the vector w mentoned above. Now the case where every graph s not connected. Lemma. [Jadbabae, Ln, Morse 003]. Let the swtched system have an nfnte sequence of contguous, nonempty, bounded tme ntervals wth the property that, acro each tme nterval the graphs are jontly connected. Then lm x( t) x. t Lemma. [Ren and Beard]. Let the swtched system have an nfnte sequence of contguous, nonempty, bounded tme ntervals wth the property that, acro each tme nterval the graphs contan a spannng tree. Then lm x( t) x. Moreover, f the unon of graphs after some fnte t tme does not have a spannng tree, consensus s not acheved n the lmt. About Lyapunov Functons for swtched graphs: There may NOT EXIST a common Lyapunov functon n such cases. Jont Lyapunov functon s too strong a requrement. Defne ut () Gt () Ltxt () () wth Gt () gi and g>n a const. Then closed-loop x( t) I L( t) x( t). system s g NOW THERE DOES EXIST a common Lyapunov Functon. If swtched graphs are jontly connected over ntervals. Remar. [Jadbabae, Ln, Morse 003]. For swtchng topologes, there may not exst a common Lyapunov functon even f consensus s reached. Moreau [005] consders DIRECTED GRAPHS. He studes the case that ncludes weghts, x( t) x( t) wjxj( t) n ( t), wth n() t wj the weghted neghbors. jn () t j Note that x( t) ( I D( t)) ( I A( t)) x( t). Ths s a stochastc matrx. In general there does not exst a tme-nvarant quadratc Lyapunov functon for ths system [Moreau 005], [Jadbabae, Ln, Morse 003]. Lemma [Moreau 005]. Drected Graphs. Let the nonzero weghts be bounded above and below. If there s a T 0 such that for all t 0 N there s a node connected to all other nodes acro [ t0, t0 T], then the N values x (t) converge to a common value as t. 3

4 Lemma [Moreau 005]. Undrected Graphs wth dfferent weghts w l w l. Let the nonzero weghts be bounded above and below. If for all t 0 N there s a node connected to all other nodes acro [ t0, ), then the N values x (t) converge to a common value. Contnuous-Tme Swtchng Models Wth swtchng, the local votng protocol for contnuous-tme systems s ut () Ltxt () () and the closed-loop system s x () t L() t x() t wth L the graph Laplacan. More specfcally ut () Lt ( ) xt (), t [ t, t ) and x () t L( t) x(), t t[ t, t ) wth t the swtchng tmes. One way to prove consensus for swtched contnuous-tme systems s to loo for jont Lyapunov functons. However, such Lyapunov functons may not exst. Another way s to consder the matrx exponental. Lemma. Let L be the Laplacan of a strongly connected dgraph. Then L has row sum of zero Lt and exactly one e-val at s=0. Moreover, s row stochastc and has exactly one e-val at z=. e Lemma. Let the swtchngs occur at tmes t such that the graph topology s constant over fnte dwell tmes t t bounded below by a postve constant. Then consensus s acheved f L( t ) L( t ) L( t ) T 0 0 lm For some vector w. e e e w Lemma. [anonymous]. A swtched gradent-based control law ut ( ) Lt ( ) xt ( ) acheves consensus asymptotcally f there exsts an nfnte sequence of bounded nonoverlappng tme ntervals wth the property that the unon of dgraphs over each nterval s strongly connected. Then, f each unon s also balanced, average consensus s solved. Lemma. [Ren and Beard 005]. The swtched CT protocol ut ( ) Lt ( ) xt ( ) acheves consensus asymptotcally f there exsts an nfnte sequence of contguous bounded tme ntervals wth the property that the unon of dgraphs over each nterval has a spannng tree. Furthermore, f the unon of graphs after some tme does not have a spannng tree, consensus cannot be acheved asymptotcally.. Communcaton Tme Delays If there are tme delays along the communcatons channels, the contnuous-tme protocol gves x () t a ( x ( t ) x ()) t j j jn 4

5 It s shown by Moreau (004) that consensus s stll acheved. However, ths protocol does not preserve the average consensus. An alternatve s to also add a desgn delay to the node s own state so that x () t a ( x ( t ) x ( t )) j j jn Then the global state dynamcs s x Lx( t ) Ths protocol does preserve the average consensus. For undrected graphs, t reaches consensus ff 0 max ( L) s See [Saber and Murray 004]. The proof reles on checng the Nyqust encrclements of Le. Note that the convergence speed of consensus depends on the smallest nonzero e-val of L, namely the Fedler e-val ( L), whle the robustne to tme delays depends on the largest e- val of L ( L). max 5

Dynamic Systems on Graphs

Dynamic Systems on Graphs Prepared by F.L. Lews Updated: Saturday, February 06, 200 Dynamc Systems on Graphs Control Graphs and Consensus A network s a set of nodes that collaborates to acheve what each cannot acheve alone. A network,

More information

A graph is a pair G= (V,E) with V a nonempty finite set of nodes or vertices V { v1 a set of edges or arcs E V V. We assume ( vi, vi) E,

A graph is a pair G= (V,E) with V a nonempty finite set of nodes or vertices V { v1 a set of edges or arcs E V V. We assume ( vi, vi) E, Prepared by FL Lews Updated: hursday, October 6, 008 Graphs A graph s a par G= (V,E) wth V a nonempty fnte set of nodes or vertces V { v,, v N } and a set of edges or arcs E V V We assume ( v, v) E,, e

More information

DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED.

DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED. EE 539 Homeworks Sprng 08 Updated: Tuesday, Aprl 7, 08 DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED. For full credt, show all work. Some problems requre hand calculatons.

More information

Random Walks on Digraphs

Random Walks on Digraphs Random Walks on Dgraphs J. J. P. Veerman October 23, 27 Introducton Let V = {, n} be a vertex set and S a non-negatve row-stochastc matrx (.e. rows sum to ). V and S defne a dgraph G = G(V, S) and a drected

More information

NP-Completeness : Proofs

NP-Completeness : Proofs NP-Completeness : Proofs Proof Methods A method to show a decson problem Π NP-complete s as follows. (1) Show Π NP. (2) Choose an NP-complete problem Π. (3) Show Π Π. A method to show an optmzaton problem

More information

Outline. Communication. Bellman Ford Algorithm. Bellman Ford Example. Bellman Ford Shortest Path [1]

Outline. Communication. Bellman Ford Algorithm. Bellman Ford Example. Bellman Ford Shortest Path [1] DYNAMIC SHORTEST PATH SEARCH AND SYNCHRONIZED TASK SWITCHING Jay Wagenpfel, Adran Trachte 2 Outlne Shortest Communcaton Path Searchng Bellmann Ford algorthm Algorthm for dynamc case Modfcatons to our algorthm

More information

Google PageRank with Stochastic Matrix

Google PageRank with Stochastic Matrix Google PageRank wth Stochastc Matrx Md. Sharq, Puranjt Sanyal, Samk Mtra (M.Sc. Applcatons of Mathematcs) Dscrete Tme Markov Chan Let S be a countable set (usually S s a subset of Z or Z d or R or R d

More information

Solutions to exam in SF1811 Optimization, Jan 14, 2015

Solutions to exam in SF1811 Optimization, Jan 14, 2015 Solutons to exam n SF8 Optmzaton, Jan 4, 25 3 3 O------O -4 \ / \ / The network: \/ where all lnks go from left to rght. /\ / \ / \ 6 O------O -5 2 4.(a) Let x = ( x 3, x 4, x 23, x 24 ) T, where the varable

More information

Continuous Time Markov Chain

Continuous Time Markov Chain Contnuous Tme Markov Chan Hu Jn Department of Electroncs and Communcaton Engneerng Hanyang Unversty ERICA Campus Contents Contnuous tme Markov Chan (CTMC) Propertes of sojourn tme Relatons Transton probablty

More information

6. Stochastic processes (2)

6. Stochastic processes (2) 6. Stochastc processes () Lect6.ppt S-38.45 - Introducton to Teletraffc Theory Sprng 5 6. Stochastc processes () Contents Markov processes Brth-death processes 6. Stochastc processes () Markov process

More information

6. Stochastic processes (2)

6. Stochastic processes (2) Contents Markov processes Brth-death processes Lect6.ppt S-38.45 - Introducton to Teletraffc Theory Sprng 5 Markov process Consder a contnuous-tme and dscrete-state stochastc process X(t) wth state space

More information

Multi-agent Consensus and Algebraic Graph Theory

Multi-agent Consensus and Algebraic Graph Theory F.L. Lews, AI Moncref-O Donnell Endowed Char Head, Controls & Sensors Group UTA Research Insttute (UTARI) The Unversty of Texas at Arlngton Mult-agent Consensus and Algebrac Graph Theory Supported by SF,

More information

EXPANSIVE MAPPINGS. by W. R. Utz

EXPANSIVE MAPPINGS. by W. R. Utz Volume 3, 978 Pages 6 http://topology.auburn.edu/tp/ EXPANSIVE MAPPINGS by W. R. Utz Topology Proceedngs Web: http://topology.auburn.edu/tp/ Mal: Topology Proceedngs Department of Mathematcs & Statstcs

More information

APPENDIX A Some Linear Algebra

APPENDIX A Some Linear Algebra APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,

More information

Containment Control for First-Order Multi-Agent Systems with Time-Varying Delays and Uncertain Topologies

Containment Control for First-Order Multi-Agent Systems with Time-Varying Delays and Uncertain Topologies Commun. heor. Phys. 66 (06) 49 55 Vol. 66, No., August, 06 Contanment Control for Frst-Order Mult-Agent Systems wth me-varyng Delays and Uncertan opologes Fu-Yong Wang ( ), Hong-Yong Yang ( ), Shu-Nng

More information

2 More examples with details

2 More examples with details Physcs 129b Lecture 3 Caltech, 01/15/19 2 More examples wth detals 2.3 The permutaton group n = 4 S 4 contans 4! = 24 elements. One s the dentty e. Sx of them are exchange of two objects (, j) ( to j and

More information

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and Ths artcle appeared n a ournal publshed by Elsever The attached copy s furnshed to the author for nternal non-commercal research and educaton use, ncludng for nstructon at the authors nsttuton and sharng

More information

Distributed Exponential Formation Control of Multiple Wheeled Mobile Robots

Distributed Exponential Formation Control of Multiple Wheeled Mobile Robots Proceedngs of the Internatonal Conference of Control, Dynamc Systems, and Robotcs Ottawa, Ontaro, Canada, May 15-16 214 Paper No. 46 Dstrbuted Exponental Formaton Control of Multple Wheeled Moble Robots

More information

Digital Signal Processing

Digital Signal Processing Dgtal Sgnal Processng Dscrete-tme System Analyss Manar Mohasen Offce: F8 Emal: manar.subh@ut.ac.r School of IT Engneerng Revew of Precedent Class Contnuous Sgnal The value of the sgnal s avalable over

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

Problem Set 9 Solutions

Problem Set 9 Solutions Desgn and Analyss of Algorthms May 4, 2015 Massachusetts Insttute of Technology 6.046J/18.410J Profs. Erk Demane, Srn Devadas, and Nancy Lynch Problem Set 9 Solutons Problem Set 9 Solutons Ths problem

More information

Singular Value Decomposition: Theory and Applications

Singular Value Decomposition: Theory and Applications Sngular Value Decomposton: Theory and Applcatons Danel Khashab Sprng 2015 Last Update: March 2, 2015 1 Introducton A = UDV where columns of U and V are orthonormal and matrx D s dagonal wth postve real

More information

U.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017

U.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017 U.C. Berkeley CS94: Beyond Worst-Case Analyss Handout 4s Luca Trevsan September 5, 07 Summary of Lecture 4 In whch we ntroduce semdefnte programmng and apply t to Max Cut. Semdefnte Programmng Recall that

More information

Tokyo Institute of Technology Periodic Sequencing Control over Multi Communication Channels with Packet Losses

Tokyo Institute of Technology Periodic Sequencing Control over Multi Communication Channels with Packet Losses oyo Insttute of echnology Fujta Laboratory oyo Insttute of echnology erodc Sequencng Control over Mult Communcaton Channels wth acet Losses FL6-7- /8/6 zwrman Gusrald oyo Insttute of echnology Fujta Laboratory

More information

Adaptive Consensus Control of Multi-Agent Systems with Large Uncertainty and Time Delays *

Adaptive Consensus Control of Multi-Agent Systems with Large Uncertainty and Time Delays * Journal of Robotcs, etworkng and Artfcal Lfe, Vol., o. (September 04), 5-9 Adaptve Consensus Control of Mult-Agent Systems wth Large Uncertanty and me Delays * L Lu School of Mechancal Engneerng Unversty

More information

Perron Vectors of an Irreducible Nonnegative Interval Matrix

Perron Vectors of an Irreducible Nonnegative Interval Matrix Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0 MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector

More information

Chapter 7 Channel Capacity and Coding

Chapter 7 Channel Capacity and Coding Chapter 7 Channel Capacty and Codng Contents 7. Channel models and channel capacty 7.. Channel models Bnary symmetrc channel Dscrete memoryless channels Dscrete-nput, contnuous-output channel Waveform

More information

Chapter 7 Channel Capacity and Coding

Chapter 7 Channel Capacity and Coding Wreless Informaton Transmsson System Lab. Chapter 7 Channel Capacty and Codng Insttute of Communcatons Engneerng atonal Sun Yat-sen Unversty Contents 7. Channel models and channel capacty 7.. Channel models

More information

REAL ANALYSIS I HOMEWORK 1

REAL ANALYSIS I HOMEWORK 1 REAL ANALYSIS I HOMEWORK CİHAN BAHRAN The questons are from Tao s text. Exercse 0.0.. If (x α ) α A s a collecton of numbers x α [0, + ] such that x α

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

Distributed Cooperative Control System Algorithms Simulations and Enhancements

Distributed Cooperative Control System Algorithms Simulations and Enhancements Po Wu and P.J. Antsakls, Dstrbuted Cooperatve Control System Algorthms: Smulatons and Enhancements, ISIS Techncal Report, Unversty of Notre Dame, ISIS-2009-001, Aprl 2009. (http://www.nd.edu/~ss/tech.html)

More information

20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The first idea is connectedness.

20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The first idea is connectedness. 20. Mon, Oct. 13 What we have done so far corresponds roughly to Chapters 2 & 3 of Lee. Now we turn to Chapter 4. The frst dea s connectedness. Essentally, we want to say that a space cannot be decomposed

More information

Distributed event-triggered coordination for average consensus on weight-balanced digraphs

Distributed event-triggered coordination for average consensus on weight-balanced digraphs Dstrbuted event-trggered coordnaton for average consensus on weght-balanced dgraphs Cameron Nowzar a Jorge Cortés b a Department of Electrcal and Systems Engneerng, Unversty of Pennsylvana, Phladelpha,

More information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

Prof. Dr. I. Nasser Phys 630, T Aug-15 One_dimensional_Ising_Model

Prof. Dr. I. Nasser Phys 630, T Aug-15 One_dimensional_Ising_Model EXACT OE-DIMESIOAL ISIG MODEL The one-dmensonal Isng model conssts of a chan of spns, each spn nteractng only wth ts two nearest neghbors. The smple Isng problem n one dmenson can be solved drectly n several

More information

Dynamic Programming. Preview. Dynamic Programming. Dynamic Programming. Dynamic Programming (Example: Fibonacci Sequence)

Dynamic Programming. Preview. Dynamic Programming. Dynamic Programming. Dynamic Programming (Example: Fibonacci Sequence) /24/27 Prevew Fbonacc Sequence Longest Common Subsequence Dynamc programmng s a method for solvng complex problems by breakng them down nto smpler sub-problems. It s applcable to problems exhbtng the propertes

More information

Continuous Time Markov Chains

Continuous Time Markov Chains Contnuous Tme Markov Chans Brth and Death Processes,Transton Probablty Functon, Kolmogorov Equatons, Lmtng Probabltes, Unformzaton Chapter 6 1 Markovan Processes State Space Parameter Space (Tme) Dscrete

More information

A class of event-triggered coordination algorithms for multi-agent systems on weight-balanced digraphs

A class of event-triggered coordination algorithms for multi-agent systems on weight-balanced digraphs 2018 Annual Amercan Control Conference (ACC) June 27 29, 2018. Wsconsn Center, Mlwaukee, USA A class of event-trggered coordnaton algorthms for mult-agent systems on weght-balanced dgraphs Png Xu Cameron

More information

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

Introduction. - The Second Lyapunov Method. - The First Lyapunov Method

Introduction. - The Second Lyapunov Method. - The First Lyapunov Method Stablty Analyss A. Khak Sedgh Control Systems Group Faculty of Electrcal and Computer Engneerng K. N. Toos Unversty of Technology February 2009 1 Introducton Stablty s the most promnent characterstc of

More information

Counterexamples to the Connectivity Conjecture of the Mixed Cells

Counterexamples to the Connectivity Conjecture of the Mixed Cells Dscrete Comput Geom 2:55 52 998 Dscrete & Computatonal Geometry 998 Sprnger-Verlag New York Inc. Counterexamples to the Connectvty Conjecture of the Mxed Cells T. Y. L and X. Wang 2 Department of Mathematcs

More information

find (x): given element x, return the canonical element of the set containing x;

find (x): given element x, return the canonical element of the set containing x; COS 43 Sprng, 009 Dsjont Set Unon Problem: Mantan a collecton of dsjont sets. Two operatons: fnd the set contanng a gven element; unte two sets nto one (destructvely). Approach: Canoncal element method:

More information

First day August 1, Problems and Solutions

First day August 1, Problems and Solutions FOURTH INTERNATIONAL COMPETITION FOR UNIVERSITY STUDENTS IN MATHEMATICS July 30 August 4, 997, Plovdv, BULGARIA Frst day August, 997 Problems and Solutons Problem. Let {ε n } n= be a sequence of postve

More information

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016 U.C. Berkeley CS94: Spectral Methods and Expanders Handout 8 Luca Trevsan February 7, 06 Lecture 8: Spectral Algorthms Wrap-up In whch we talk about even more generalzatons of Cheeger s nequaltes, and

More information

Genericity of Critical Types

Genericity of Critical Types Genercty of Crtcal Types Y-Chun Chen Alfredo D Tllo Eduardo Fangold Syang Xong September 2008 Abstract Ely and Pesk 2008 offers an nsghtful characterzaton of crtcal types: a type s crtcal f and only f

More information

Appendix B. Criterion of Riemann-Stieltjes Integrability

Appendix B. Criterion of Riemann-Stieltjes Integrability Appendx B. Crteron of Remann-Steltes Integrablty Ths note s complementary to [R, Ch. 6] and [T, Sec. 3.5]. The man result of ths note s Theorem B.3, whch provdes the necessary and suffcent condtons for

More information

Distributed Multi-Agent Coordination: A Comparison Lemma Based Approach

Distributed Multi-Agent Coordination: A Comparison Lemma Based Approach 2011 Amercan Control Conference on O'Farrell Street, San Francsco, CA, USA June 29 - July 01, 2011 Dstrbuted Mult-Agent Coordnaton: A Comparson Lemma Based Approach Yongcan Cao and We Ren Abstract In ths

More information

Zeros and Zero Dynamics for Linear, Time-delay System

Zeros and Zero Dynamics for Linear, Time-delay System UNIVERSITA POLITECNICA DELLE MARCHE - FACOLTA DI INGEGNERIA Dpartmento d Ingegnerua Informatca, Gestonale e dell Automazone LabMACS Laboratory of Modelng, Analyss and Control of Dynamcal System Zeros and

More information

Outline and Reading. Dynamic Programming. Dynamic Programming revealed. Computing Fibonacci. The General Dynamic Programming Technique

Outline and Reading. Dynamic Programming. Dynamic Programming revealed. Computing Fibonacci. The General Dynamic Programming Technique Outlne and Readng Dynamc Programmng The General Technque ( 5.3.2) -1 Knapsac Problem ( 5.3.3) Matrx Chan-Product ( 5.3.1) Dynamc Programmng verson 1.4 1 Dynamc Programmng verson 1.4 2 Dynamc Programmng

More information

A new construction of 3-separable matrices via an improved decoding of Macula s construction

A new construction of 3-separable matrices via an improved decoding of Macula s construction Dscrete Optmzaton 5 008 700 704 Contents lsts avalable at ScenceDrect Dscrete Optmzaton journal homepage: wwwelsevercom/locate/dsopt A new constructon of 3-separable matrces va an mproved decodng of Macula

More information

Formation Flight Control of Multi-UAV System with Communication Constraints

Formation Flight Control of Multi-UAV System with Communication Constraints do: 105028/jatmv8208 Formaton Flght Control of Mult-UAV System wth Communcaton Constrants Rubn Xue 1, Gaohua Ca 2 Abstract: Three dmensonal formaton control problem of mult-uav system wth communcaton constrants

More information

Multi-dimensional Central Limit Theorem

Multi-dimensional Central Limit Theorem Mult-dmensonal Central Lmt heorem Outlne ( ( ( t as ( + ( + + ( ( ( Consder a sequence of ndependent random proceses t, t, dentcal to some ( t. Assume t = 0. Defne the sum process t t t t = ( t = (; t

More information

Non-negative Matrices and Distributed Control

Non-negative Matrices and Distributed Control Non-negatve Matrces an Dstrbute Control Yln Mo July 2, 2015 We moel a network compose of m agents as a graph G = {V, E}. V = {1, 2,..., m} s the set of vertces representng the agents. E V V s the set of

More information

Convergence of random processes

Convergence of random processes DS-GA 12 Lecture notes 6 Fall 216 Convergence of random processes 1 Introducton In these notes we study convergence of dscrete random processes. Ths allows to characterze phenomena such as the law of large

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

Statistical Mechanics and Combinatorics : Lecture III

Statistical Mechanics and Combinatorics : Lecture III Statstcal Mechancs and Combnatorcs : Lecture III Dmer Model Dmer defntons Defnton A dmer coverng (perfect matchng) of a fnte graph s a set of edges whch covers every vertex exactly once, e every vertex

More information

STAT 309: MATHEMATICAL COMPUTATIONS I FALL 2018 LECTURE 16

STAT 309: MATHEMATICAL COMPUTATIONS I FALL 2018 LECTURE 16 STAT 39: MATHEMATICAL COMPUTATIONS I FALL 218 LECTURE 16 1 why teratve methods f we have a lnear system Ax = b where A s very, very large but s ether sparse or structured (eg, banded, Toepltz, banded plus

More information

Lecture 3: Probability Distributions

Lecture 3: Probability Distributions Lecture 3: Probablty Dstrbutons Random Varables Let us begn by defnng a sample space as a set of outcomes from an experment. We denote ths by S. A random varable s a functon whch maps outcomes nto the

More information

Modelli Clamfim Equazione del Calore Lezione ottobre 2014

Modelli Clamfim Equazione del Calore Lezione ottobre 2014 CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g

More information

Exercise Solutions to Real Analysis

Exercise Solutions to Real Analysis xercse Solutons to Real Analyss Note: References refer to H. L. Royden, Real Analyss xersze 1. Gven any set A any ɛ > 0, there s an open set O such that A O m O m A + ɛ. Soluton 1. If m A =, then there

More information

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class

More information

DS-GA 1002 Lecture notes 5 Fall Random processes

DS-GA 1002 Lecture notes 5 Fall Random processes DS-GA Lecture notes 5 Fall 6 Introducton Random processes Random processes, also known as stochastc processes, allow us to model quanttes that evolve n tme (or space n an uncertan way: the trajectory of

More information

Fixed point. The function q revisited. Function q. graph F factorial graph factorial. factorial is a fixed point of F, since

Fixed point. The function q revisited. Function q. graph F factorial graph factorial. factorial is a fixed point of F, since CS571 Notes 21 Denotatonal Semantcs of Loops (contnued 1of 25 Generalzng the soluton Parameterze the factoral functon F = λ f.λ n. n equals zero one n tmes ( f ( n mnus one Ths means fac = + 1 F ( fac.e.

More information

Improved delay-dependent stability criteria for discrete-time stochastic neural networks with time-varying delays

Improved delay-dependent stability criteria for discrete-time stochastic neural networks with time-varying delays Avalable onlne at www.scencedrect.com Proceda Engneerng 5 ( 4456 446 Improved delay-dependent stablty crtera for dscrete-tme stochastc neural networs wth tme-varyng delays Meng-zhuo Luo a Shou-mng Zhong

More information

Digital Modems. Lecture 2

Digital Modems. Lecture 2 Dgtal Modems Lecture Revew We have shown that both Bayes and eyman/pearson crtera are based on the Lkelhood Rato Test (LRT) Λ ( r ) < > η Λ r s called observaton transformaton or suffcent statstc The crtera

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

This model contains two bonds per unit cell (one along the x-direction and the other along y). So we can rewrite the Hamiltonian as:

This model contains two bonds per unit cell (one along the x-direction and the other along y). So we can rewrite the Hamiltonian as: 1 Problem set #1 1.1. A one-band model on a square lattce Fg. 1 Consder a square lattce wth only nearest-neghbor hoppngs (as shown n the fgure above): H t, j a a j (1.1) where,j stands for nearest neghbors

More information

Asynchronous Periodic Event-Triggered Coordination of Multi-Agent Systems

Asynchronous Periodic Event-Triggered Coordination of Multi-Agent Systems 017 IEEE 56th Annual Conference on Decson and Control (CDC) December 1-15, 017, Melbourne, Australa Asynchronous Perodc Event-Trggered Coordnaton of Mult-Agent Systems Yaohua Lu Cameron Nowzar Zh Tan Qng

More information

Strong Markov property: Same assertion holds for stopping times τ.

Strong Markov property: Same assertion holds for stopping times τ. Brownan moton Let X ={X t : t R + } be a real-valued stochastc process: a famlty of real random varables all defned on the same probablty space. Defne F t = nformaton avalable by observng the process up

More information

Neuro-Adaptive Design - I:

Neuro-Adaptive Design - I: Lecture 36 Neuro-Adaptve Desgn - I: A Robustfyng ool for Dynamc Inverson Desgn Dr. Radhakant Padh Asst. Professor Dept. of Aerospace Engneerng Indan Insttute of Scence - Bangalore Motvaton Perfect system

More information

Composite Hypotheses testing

Composite Hypotheses testing Composte ypotheses testng In many hypothess testng problems there are many possble dstrbutons that can occur under each of the hypotheses. The output of the source s a set of parameters (ponts n a parameter

More information

CSCE 790S Background Results

CSCE 790S Background Results CSCE 790S Background Results Stephen A. Fenner September 8, 011 Abstract These results are background to the course CSCE 790S/CSCE 790B, Quantum Computaton and Informaton (Sprng 007 and Fall 011). Each

More information

Consensus of Multi-Agent Systems by Distributed Event-Triggered Control

Consensus of Multi-Agent Systems by Distributed Event-Triggered Control Preprnts of the 19th World Congress The Internatonal Federaton of Automatc Control Consensus of Mult-Agent Systems by Dstrbuted Event-Trggered Control Wenfeng Hu, Lu Lu, Gang Feng Department of Mechancal

More information

EEE 241: Linear Systems

EEE 241: Linear Systems EEE : Lnear Systems Summary #: Backpropagaton BACKPROPAGATION The perceptron rule as well as the Wdrow Hoff learnng were desgned to tran sngle layer networks. They suffer from the same dsadvantage: they

More information

TAIL BOUNDS FOR SUMS OF GEOMETRIC AND EXPONENTIAL VARIABLES

TAIL BOUNDS FOR SUMS OF GEOMETRIC AND EXPONENTIAL VARIABLES TAIL BOUNDS FOR SUMS OF GEOMETRIC AND EXPONENTIAL VARIABLES SVANTE JANSON Abstract. We gve explct bounds for the tal probabltes for sums of ndependent geometrc or exponental varables, possbly wth dfferent

More information

The lower and upper bounds on Perron root of nonnegative irreducible matrices

The lower and upper bounds on Perron root of nonnegative irreducible matrices Journal of Computatonal Appled Mathematcs 217 (2008) 259 267 wwwelsevercom/locate/cam The lower upper bounds on Perron root of nonnegatve rreducble matrces Guang-Xn Huang a,, Feng Yn b,keguo a a College

More information

How to Stop Consensus Algorithms, locally?

How to Stop Consensus Algorithms, locally? 1 How to Stop Consensus Algorthms, locally? Pe Xe, Keyou You and Cheng Wu arxv:1703.05106v1 [cs.dc] 15 Mar 2017 Abstract Ths paper studes problems on locally stoppng dstrbuted consensus algorthms over

More information

Multi-dimensional Central Limit Argument

Multi-dimensional Central Limit Argument Mult-dmensonal Central Lmt Argument Outlne t as Consder d random proceses t, t,. Defne the sum process t t t t () t (); t () t are d to (), t () t 0 () t tme () t () t t t As, ( t) becomes a Gaussan random

More information

MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS

MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS These are nformal notes whch cover some of the materal whch s not n the course book. The man purpose s to gve a number of nontrval examples

More information

Maximizing the number of nonnegative subsets

Maximizing the number of nonnegative subsets Maxmzng the number of nonnegatve subsets Noga Alon Hao Huang December 1, 213 Abstract Gven a set of n real numbers, f the sum of elements of every subset of sze larger than k s negatve, what s the maxmum

More information

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1

C/CS/Phy191 Problem Set 3 Solutions Out: Oct 1, 2008., where ( 00. ), so the overall state of the system is ) ( ( ( ( 00 ± 11 ), Φ ± = 1 C/CS/Phy9 Problem Set 3 Solutons Out: Oct, 8 Suppose you have two qubts n some arbtrary entangled state ψ You apply the teleportaton protocol to each of the qubts separately What s the resultng state obtaned

More information

Differentiating Gaussian Processes

Differentiating Gaussian Processes Dfferentatng Gaussan Processes Andrew McHutchon Aprl 17, 013 1 Frst Order Dervatve of the Posteror Mean The posteror mean of a GP s gven by, f = x, X KX, X 1 y x, X α 1 Only the x, X term depends on the

More information

Math1110 (Spring 2009) Prelim 3 - Solutions

Math1110 (Spring 2009) Prelim 3 - Solutions Math 1110 (Sprng 2009) Solutons to Prelm 3 (04/21/2009) 1 Queston 1. (16 ponts) Short answer. Math1110 (Sprng 2009) Prelm 3 - Solutons x a 1 (a) (4 ponts) Please evaluate lm, where a and b are postve numbers.

More information

FINITE-STATE MARKOV CHAINS

FINITE-STATE MARKOV CHAINS Chapter 4 FINITE-STATE MARKOV CHAINS 4.1 Introducton The countng processes {N(t), t 0} of Chapterss 2 and 3 have the property that N(t) changes at dscrete nstants of tme, but s defned for all real t 0.

More information

Computing Correlated Equilibria in Multi-Player Games

Computing Correlated Equilibria in Multi-Player Games Computng Correlated Equlbra n Mult-Player Games Chrstos H. Papadmtrou Presented by Zhanxang Huang December 7th, 2005 1 The Author Dr. Chrstos H. Papadmtrou CS professor at UC Berkley (taught at Harvard,

More information

Lecture Notes on Linear Regression

Lecture Notes on Linear Regression Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume

More information

7. Products and matrix elements

7. Products and matrix elements 7. Products and matrx elements 1 7. Products and matrx elements Based on the propertes of group representatons, a number of useful results can be derved. Consder a vector space V wth an nner product ψ

More information

10-701/ Machine Learning, Fall 2005 Homework 3

10-701/ Machine Learning, Fall 2005 Homework 3 10-701/15-781 Machne Learnng, Fall 2005 Homework 3 Out: 10/20/05 Due: begnnng of the class 11/01/05 Instructons Contact questons-10701@autonlaborg for queston Problem 1 Regresson and Cross-valdaton [40

More information

Spectral graph theory: Applications of Courant-Fischer

Spectral graph theory: Applications of Courant-Fischer Spectral graph theory: Applcatons of Courant-Fscher Steve Butler September 2006 Abstract In ths second talk we wll ntroduce the Raylegh quotent and the Courant- Fscher Theorem and gve some applcatons for

More information

MEM633 Lectures 7&8. Chapter 4. Descriptions of MIMO Systems 4-1 Direct Realizations. (i) x u. y x

MEM633 Lectures 7&8. Chapter 4. Descriptions of MIMO Systems 4-1 Direct Realizations. (i) x u. y x MEM633 Lectures 7&8 Chapter 4 Descrptons of MIMO Systems 4- Drect ealzatons y() s s su() s y () s u () s ( s)( s) s y() s u (), s y() s u() s s s y() s u(), s y() s u() s ( s)( s) s () ( s ) y ( s) u (

More information

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets

where a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets 11. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

Complete subgraphs in multipartite graphs

Complete subgraphs in multipartite graphs Complete subgraphs n multpartte graphs FLORIAN PFENDER Unverstät Rostock, Insttut für Mathematk D-18057 Rostock, Germany Floran.Pfender@un-rostock.de Abstract Turán s Theorem states that every graph G

More information

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)? Homework 8 solutons. Problem 16.1. Whch of the followng defne homomomorphsms from C\{0} to C\{0}? Answer. a) f 1 : z z Yes, f 1 s a homomorphsm. We have that z s the complex conjugate of z. If z 1,z 2

More information

Degree Fluctuations and the Convergence Time of Consensus Algorithms

Degree Fluctuations and the Convergence Time of Consensus Algorithms Degree Fluctuatons and the Convergence Tme of Consensus Algorthms Alex Olshevsy John N. Tstsls Abstract We consder a consensus algorthm n whch every node n a tme-varyng undrected connected graph assgns

More information

Lecture 10: May 6, 2013

Lecture 10: May 6, 2013 TTIC/CMSC 31150 Mathematcal Toolkt Sprng 013 Madhur Tulsan Lecture 10: May 6, 013 Scrbe: Wenje Luo In today s lecture, we manly talked about random walk on graphs and ntroduce the concept of graph expander,

More information

Decentralized Event-Triggered Cooperative Control with Limited Communication

Decentralized Event-Triggered Cooperative Control with Limited Communication Decentralzed Event-Trggered Cooperatve Control wth Lmted Communcaton Abstract Ths note studes event-trggered control of Mult-Agent Systems (MAS) wth frst order ntegrator dynamcs. It extends prevous work

More information

The Feynman path integral

The Feynman path integral The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space

More information