Lecture 22. Lecturer: Michel X. Goemans Scribe: Alantha Newman (2004), Ankur Moitra (2009)
|
|
- Myron Howard
- 6 years ago
- Views:
Transcription
1 8.438 Avance Combinatorial Optimization Lecture Lecturer: Michel X. Goemans Scribe: Alantha Newman (004), Ankur Moitra (009) MultiFlows an Disjoint Paths Here we will survey a number of variants of isjoint path problems, an give reuctions between these ifferent variants. We will also consier fractional relaxations of these problems, an in the special case of two source-sink pairs, we will prove a max-flow min-cut relation an in fact in this case, this flow can even be realize half-integrally.. Notation We will consier isjoint path problems in both irecte, an unirecte graphs. Aitionally, we will consier both ege-isjoint an vertex-isjoint paths problems. In the case of a igraph, we will let D = (V, A) be the igraph an we will enote the set of arcs by A. In the case of an unirecte graph, we will use G = (V, E) to enote the set of eges by E. Let s, t, s, t,... s k, t k V be terminals. Our goal is to fin isjoint paths between s i an t i for each i, i k. Again, the notion of path an the notion of isjoint epens on the variant of the isjoint path problem that we are consiering. We can in fact consier a more general problem, in which each pair of terminals s i, t i is also given an integer eman i, an our goal is to connect every source-sink pair s i, t i by i paths, an all paths connecting any source-sink pair must be isjoint. We can also generalize this question further, by allowing capacities on eges in the case of ege isjoint path problems. Here we are also given a capacity function c : A Z + or c : E Z + an our goal is again to connect each pair of terminals s i, t i by i paths, subject to the constraints that each (arc or) ege e is use at most c(e) times. So we can interpret the capacity on an (arc or) ege as a boun on the number of paths that are allowe to traverse this ege. Or we can even relax this further an consier a collection of (possibly non-integral) flows, which collectively satisfy the capacity constraints an such that the ith flow has i units between s i an t i. In the case of just a single source-sink pair s, t an integer eman, this problem is wellunerstoo: Let f be the maximum number of paths connecting s, t (subject to capacity constraints) in G = (V, E) (or in a igraph D = (V, A)). Then f is equal to the capacity of the minimum cut separating s from t. But for many source-sink pairs, the minimum cut is no longer equal to the maximum number of paths (subject to capacity constraints). In fact, each of the variants of the isjoint paths problem mentione above is NP -har, but the ifficulty of these problems is quite ifferent.. Directe an Unirecte Ege Disjoint Paths The unirecte an irecte ege isjoint path problems are rastically ifferent for a fixe number of source-sink pairs: Unirecte Ege Disjoint Paths. In the case of fixe k (i.e. there are k source-sink pairs), there is a polynomial time algorithm to ecie if there are ege isjoint paths connecting each s i, t i pair. This result follows from the Graph Minor Project of Robertson an Seymour (995), an is very involve. Yet for super-constant k, the unirecte ege isjoint paths problem is N P -complete. -
2 Directe Arc Disjoint Paths. Even for k = it is NP -complete to etermine if there are arc-isjoint paths P, P connecting s, t an s, t. In fact, we can even choose s = t an s = t an this problem still remains N P -complete. This rastic ifference in the range for which these problems are har, leas to very ifferent inapproximability results. For the problems of maximizing the number of arc-isjoint paths, in the case of a irecte graph, it is har to etermine the maximum number of arc-isjoint paths within any Ω(m ɛ ) for m arcs, an for any ɛ > 0. Yet for the case of maximizing the number of ege isjoint paths in an unirecte graph, the best known harness results are only poly-logarithmic. An in either case, the best known approximation ratio is O( m) (or actually O( n) for unirecte graphs on n vertices)..3 Reuctions Between Variants Here we consier all four problems, (unirecte or irecte) (ege or vertex) isjoint paths. We first note that the arc-isjoint path problem, an the vertex-isjoint path problem in a irecte graph are equivalent - i.e. we can give a polynomial time reuction in either irection. Given a vertex-isjoint path problem in a irecte graph, we can perform the reuction in Figure an get a are-isjoint path problem that is equivalent. Figure : Each vertex unergoes the illustrate transformation. In the case of an arc-isjoint path problem, we can perform a similar transformation given in Figure. Figure : Each vertex unergoes the illustrate transformation. Next we consier reuctions from unirecte variants of the isjoint path problem, an prove that both the ege isjoint path problem an the vertex-isjoint path problem (in unirecte graphs) can be reuce to either irecte path problem above. We can also reuce the ege isjoint path problem in unirecte graphs to the arc-isjoint path problem, an this reuction is given in Figure 3. This also implies that we can reuce the ege isjoint path problem in unirecte graphs to the irecte vertex-isjoint path problem. a b a b Figure 3: Each ege in the original unirecte graph is replace by the above gaget. -
3 For the case of the vertex isjoint path problem in unirecte graphs, we can just replace any ege (u, v) by two arcs (u, v) an (v, u). So this problem can also be reuce to either the arc-isjoint path problem or the vertex-isjoint path problem in irecte graphs. Lastly, the ege isjoint path problem in unirecte graphs can be reuce to the vertex-isjoint path problem in unirecte graphs by taking the line-graph of G. A path in the line-graph of G will also correspon to a path in the original graph G, but vertices in the line-graph correspon to eges in the original graph, so paths will be ege-isjoint in G iff the corresponing paths are vertex-isjoint in the line graph of G..4 Fractional Relaxations We focus on ege isjoint paths in unirecte graphs. When k =, flow is easy. We can fin integer flow using the max-flow min-cut theorem. In general, we can give a fractional relaxation (that can be solve because it can be written as a linear program): Let P i be set of all paths between s i an t i. We have a variable x p for every such path p P i. We have the following primal LP: max 0 x x p = i p P i x p c(e) i:p P i,e p x p 0. What oes ual mean in this case? We use variables l(e) for each ege e E, an variables b i for i =,..., k. min e E c(e)l(e) k b i i () i= l(e) b i 0 p P i i =,... k e p l(e) 0. To make the term ( k i= b i i ) small, we shoul make b i as large as possible. Fix the ege function l : E Q. Then b i is the (minimum) ist l (s i, t i ). The objective function of the ual () can be rewritten: c(e)l(e) e E k i ist l (s i, t i ). i= If the primal LP is feasible, then there is no solution for the ual LP with a negative objective value. So there exists a fractional multiflow if an only if l(e) 0, e E, the following hols: k c(e)l(e) i ist l (s i, t i ). () e E i= Duality shows that this is a necessary an sufficient for the existence of a fractional multiflow. -3
4 Integer Multiflows In general, the problem of etermining when there is an integer multiflow is NP-complete. However, there are special conitions that imply the existence of an integer multiflow in certain classes of graphs. Let R be a set of eges: R = {(s i, t i ) : i =,... k}. (3) The set of eges in E outgoing from vertex set U is enote by δ E (U) an the set of eges in R outgoing from vertex set U is enote by δ R (U). A necessary conition for the existence of a multiflow (an thus of an integer multiflow) is the cut conition: c(δ E (U)) (δ R (U)), U V. In general, the cut conition is not sufficient to guarantee the existence of an integer multiflow (or fractional multiflow) in a graph. However, in some cases of the multiflow problem, the cut conition is sufficient for the existence of a fractional multiflow. Furthermore, there are several cases known where the cut conition implies the existence of an integer multiflow when the Euler conition is satisfie: c(δ E (v)) + (δ R (v)) is even, for each vertex v. For example, when k =, we have the following implications: (i) Cut conition fractional multiflow. (ii) Cut conition an integer capacities half-integral multiflow. (iii) Cut conition, integer capacities, an Euler conition integral multiflow. s t s t Figure 4: When the capacity of each ege in this graph is an, =, the Euler conition is not satisfie. There exists a half-integral multiflow, but no integral multiflow. The first proof of (i) an (ii) for the case when k = was is ue to Hu. The proof of (iii) is ue to Rothschil an Winston. Note that (iii) implies (i) an (ii). For example, Consier the graph in Figure 4, let =, =. Let the capacity of each ege be. Note that the cut conition is satisfie but the Euler conition is not. However, suppose we ouble every capacity an eman, then the Euler conition is satisfie. We can convert an integer solution for this latter problem to a half-integral solution for the original problem. Some goo cases in which conitions (i), (ii) an (iii) are satisfie are: -4
5 . If there are two commoities, i.e. k =, then cut conition an Euler conition are sufficient for integer multiflow.. G + D has no K 5 minor, (a special case is when G + D is planar) where D is the eman graph, D = (V, R) (see (3)). 3. {(s, t ),..., (s k, t k )} G is planar an all (s i, t i ) are on bounary of outsie face. (Note that this oes not imply case because the eman graph coul be a clique) 5. If there are faces F, F an for each i, (s i, t i ) are both on the bounary of the same face F j for j {, }. 3 Two-Commoity Flows Theorem (Rothschil an Whinston) G = (V, E) is an unirecte graph such that c(e) Z + for e E. Terminals s, t, s, t are in V, an emans, are positive integers. Aitionally, the Euler conition is satisfie for G. Then G has an integer two-commoity flow if an only if the cut conition is satisfie. Proof: Our goal is to fin flows from s to t an from s to t with values an, respectively. We will show that if the cut conition is satisfie on G, then we can fin such flows. G : s s t s t t G : s s t t s t Figure 5: The graphs G an G are constructe base on the given graph G. First, base on the graph G, construct the graph G as shown in Figure 5. Note that the eges out of s are the only irecte eges in the graph G, an all other eges are inherite from G an hence unirecte. Let the eges (s, s ) an (t, t ) in G have capacity an the eges (s, s ) an (t, t ) in G have capacity. By the max-flow min-cut theorem, we can fin an integer s -t flow g with value +, since the min-cut of G has value +. Note that this s -t flow oes not necessarily give a two-commoity flow for the original problem (since some of the flow going through s may en up in t ). Since the Euler conition is satisfie, we will prove that we can assume that g(e) c(e) mo. To show this, first notice that the Euler conition implies that the total capacity incient to any vertex (except s or t ) of G is even. Furthermore, any integral flow will use up an even amount of capacity incient to any vertex. Now consier all the eges e E such that g(e) c(e) mo. Since it is the case that e δ(v) (g(e) c(e)) = 0 mo, it follows that an even number of eges ajacent to vertex v have g(e) c(e) mo. Thus, the eges such that g(e) c(e) mo make up an Eulerian graph (an o not contain the arcs incient to s an t that we ae to G to make up G, as these arcs are saturate). We can ecompose this Eulerian graph into cycles, an push push one unit of flow across all these cycles (either increasing or ecreasing the flow by one unit -5
6 along it epening on the orientation), changing the parity of g(e) for each such ege. Thus, for all eges e E, we have that g(e) c(e) mo. For G, we have the same argument. Thus, we fin an integer flow h in G with value + such that h(e) = c(e) mo, e E. Thus, for all eges e E, h(e) = g(e) mo. We arbitrarily orient the eges of E to obtain A. So for all a A, h(a) g(a) mo. Now we efine two flows on the graph G: f (a) = [g(a) + h(a)] f (a) = [g(a) h(a)]. The following properties are true for the flows f an f :. f (a), f (a) are integer flows (since g(a) an h(a) have the same parity).. f (a) + f (a) = g(a) + h(a) + g(a) h(a) max( g(a), h(a) ) c(a). 3. f is units of flow from s to t an f is units of flow from s to t. The last property hols because we can show that f (δ + (s )) f (δ (s )) = an f (δ (t )) f (δ + (t )) =. By conservation of flow, if we consier the vertex s in G, we have: Equations (4) an (5) imply f (δ + (s )) f (δ (s )) =. g(δ + (s )) g(δ (s )) = (4) h(δ + (s )) h(δ (s )) = (5) g(δ (t )) g(δ + (t )) = (6) h(δ (t )) h(δ + (t )) =. (7) Equations (6) an (7) imply f (δ (t )) f (δ + (t )) =. Similarly, we can show that the last property hols for flow f. If we consier vertices s an t in G, we have: g(δ + (s )) g(δ (s )) = (8) h(δ (s )) h(δ + (s )) = (9) g(δ (t )) g(δ + (t )) = (0) h(δ + (t )) h(δ (t )) =. () Equations (8) an (9) imply f (δ + (s )) f (δ (s )) = f (δ (t )) f (δ + (s )) =. an equations (0) an () imply As a final note, consier the problem of maximizing the sum of the flow between s an t an between s an t. This is the max biflow problem. A bicut is a cut separating s from t an s from t, thus it is either a cut separating s, s from t, t or a cut separating s, t from s, t. One can show that the following theorem follows from Theorem. Theorem The maximum biflow equals the minimum bicut. -6
Topics in Combinatorial Optimization May 11, Lecture 22
8.997 Topics in Combinaorial Opimizaion May, 004 Lecure Lecurer: Michel X. Goemans Scribe: Alanha Newman Muliflows an Disjoin Pahs Le G = (V,E) be a graph an le s,,s,,...s, V be erminals. Our goal is o
More informationLecture 5. Symmetric Shearer s Lemma
Stanfor University Spring 208 Math 233: Non-constructive methos in combinatorics Instructor: Jan Vonrák Lecture ate: January 23, 208 Original scribe: Erik Bates Lecture 5 Symmetric Shearer s Lemma Here
More informationLower Bounds for the Smoothed Number of Pareto optimal Solutions
Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.
More informationPermanent vs. Determinant
Permanent vs. Determinant Frank Ban Introuction A major problem in theoretical computer science is the Permanent vs. Determinant problem. It asks: given an n by n matrix of ineterminates A = (a i,j ) an
More informationA Sketch of Menshikov s Theorem
A Sketch of Menshikov s Theorem Thomas Bao March 14, 2010 Abstract Let Λ be an infinite, locally finite oriente multi-graph with C Λ finite an strongly connecte, an let p
More informationOn colour-blind distinguishing colour pallets in regular graphs
J Comb Optim (2014 28:348 357 DOI 10.1007/s10878-012-9556-x On colour-blin istinguishing colour pallets in regular graphs Jakub Przybyło Publishe online: 25 October 2012 The Author(s 2012. This article
More informationCMSC 858F: Algorithmic Game Theory Fall 2010 BGP and Interdomain Routing
CMSC 858F: Algorithmic Game Theory Fall 2010 BGP an Interomain Routing Instructor: Mohamma T. Hajiaghayi Scribe: Yuk Hei Chan November 3, 2010 1 Overview In this lecture, we cover BGP (Borer Gateway Protocol)
More information- Well-characterized problems, min-max relations, approximate certificates. - LP problems in the standard form, primal and dual linear programs
LP-Duality ( Approximation Algorithms by V. Vazirani, Chapter 12) - Well-characterized problems, min-max relations, approximate certificates - LP problems in the standard form, primal and dual linear programs
More informationMcMaster University. Advanced Optimization Laboratory. Title: The Central Path Visits all the Vertices of the Klee-Minty Cube.
McMaster University Avance Optimization Laboratory Title: The Central Path Visits all the Vertices of the Klee-Minty Cube Authors: Antoine Deza, Eissa Nematollahi, Reza Peyghami an Tamás Terlaky AvOl-Report
More informationCombinatorica 9(1)(1989) A New Lower Bound for Snake-in-the-Box Codes. Jerzy Wojciechowski. AMS subject classification 1980: 05 C 35, 94 B 25
Combinatorica 9(1)(1989)91 99 A New Lower Boun for Snake-in-the-Box Coes Jerzy Wojciechowski Department of Pure Mathematics an Mathematical Statistics, University of Cambrige, 16 Mill Lane, Cambrige, CB2
More informationMath 342 Partial Differential Equations «Viktor Grigoryan
Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite
More informationCalculus of Variations
16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t
More informationTable of Common Derivatives By David Abraham
Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec
More informationPDE Notes, Lecture #11
PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =
More informationIterated Point-Line Configurations Grow Doubly-Exponentially
Iterate Point-Line Configurations Grow Doubly-Exponentially Joshua Cooper an Mark Walters July 9, 008 Abstract Begin with a set of four points in the real plane in general position. A to this collection
More informationMath 115 Section 018 Course Note
Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of
More informationExact Max 2-Sat: Easier and Faster
Exact Max -Sat: Easier an Faster Martin Fürer Shiva Prasa Kasiviswanathan Computer Science an Engineering, Pennsylvania State University e-mail: {furer,kasivisw}@cse.psu.eu Abstract Prior algorithms known
More informationPhysics 2212 K Quiz #2 Solutions Summer 2016
Physics 1 K Quiz # Solutions Summer 016 I. (18 points) A positron has the same mass as an electron, but has opposite charge. Consier a positron an an electron at rest, separate by a istance = 1.0 nm. What
More informationBIRS Ron Peled (Tel Aviv University) Portions joint with Ohad N. Feldheim (Tel Aviv University)
2.6.2011 BIRS Ron Pele (Tel Aviv University) Portions joint with Oha N. Felheim (Tel Aviv University) Surface: f : Λ Hamiltonian: H(f) DGFF: V f(x) f(y) x~y V(x) x 2. R or for f a Λ a box Ranom surface:
More informationPerfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs
Perfect Matchings in Õ(n1.5 ) Time in Regular Bipartite Graphs Ashish Goel Michael Kapralov Sanjeev Khanna Abstract We consier the well-stuie problem of fining a perfect matching in -regular bipartite
More informationSchrödinger s equation.
Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of
More informationLecture 2 Lagrangian formulation of classical mechanics Mechanics
Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,
More informationThe Inapproximability of Maximum Single-Sink Unsplittable, Priority and Confluent Flow Problems
The Inapproximability of Maximum Single-Sink Unsplittable, Priority and Confluent Flow Problems arxiv:1504.00627v2 [cs.ds] 15 May 2015 F. Bruce Shepherd Adrian Vetta August 20, 2018 Abstract We consider
More informationOn Pathos Lict Subdivision of a Tree
International J.Math. Combin. Vol.4 (010), 100-107 On Pathos Lict Subivision of a Tree Keerthi G.Mirajkar an Iramma M.Kaakol (Department of Mathematics, Karnatak Arts College, Dharwa-580 001, Karnataka,
More informationUNDERSTANDING INTEGRATION
UNDERSTANDING INTEGRATION Dear Reaer The concept of Integration, mathematically speaking, is the "Inverse" of the concept of result, the integration of, woul give us back the function f(). This, in a way,
More informationmodel considered before, but the prey obey logistic growth in the absence of predators. In
5.2. First Orer Systems of Differential Equations. Phase Portraits an Linearity. Section Objective(s): Moifie Preator-Prey Moel. Graphical Representations of Solutions. Phase Portraits. Vector Fiels an
More informationLecture 12: November 6, 2013
Information an Coing Theory Autumn 204 Lecturer: Mahur Tulsiani Lecture 2: November 6, 203 Scribe: Davi Kim Recall: We were looking at coes of the form C : F k q F n q, where q is prime, k is the message
More informationQuantum Mechanics in Three Dimensions
Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.
More informationθ x = f ( x,t) could be written as
9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)
More information1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.
Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency
More information26.1 Metropolis method
CS880: Approximations Algorithms Scribe: Dave Anrzejewski Lecturer: Shuchi Chawla Topic: Metropolis metho, volume estimation Date: 4/26/07 The previous lecture iscusse they some of the key concepts of
More informationThe Complexity of Recognizing Tough Cubic Graphs
The Complexity of Recognizing Tough Cubic Graphs D. auer 1 J. van en Heuvel 2 A. Morgana 3 E. Schmeichel 4 1 Department of Mathematical Sciences, Stevens Institute of Technology Hoboken, NJ 07030, U.S.A.
More informationFinal Exam Study Guide and Practice Problems Solutions
Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making
More informationGoal of this chapter is to learn what is Capacitance, its role in electronic circuit, and the role of dielectrics.
PHYS 220, Engineering Physics, Chapter 24 Capacitance an Dielectrics Instructor: TeYu Chien Department of Physics an stronomy University of Wyoming Goal of this chapter is to learn what is Capacitance,
More informationSolutions to MATH 271 Test #3H
Solutions to MATH 71 Test #3H This is the :4 class s version of the test. See pages 4 7 for the 4:4 class s. (1) (5 points) Let a k = ( 1)k. Is a k increasing? Decreasing? Boune above? Boune k below? Convergant
More informationLinear and quadratic approximation
Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function
More informationOn the enumeration of partitions with summands in arithmetic progression
AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics
More informationTHE ACCURATE ELEMENT METHOD: A NEW PARADIGM FOR NUMERICAL SOLUTION OF ORDINARY DIFFERENTIAL EQUATIONS
THE PUBISHING HOUSE PROCEEDINGS O THE ROMANIAN ACADEMY, Series A, O THE ROMANIAN ACADEMY Volume, Number /, pp. 6 THE ACCURATE EEMENT METHOD: A NEW PARADIGM OR NUMERICA SOUTION O ORDINARY DIERENTIA EQUATIONS
More informationLarge Triangles in the d-dimensional Unit-Cube (Extended Abstract)
Large Triangles in the -Dimensional Unit-Cube Extene Abstract) Hanno Lefmann Fakultät für Informatik, TU Chemnitz, D-0907 Chemnitz, Germany lefmann@informatik.tu-chemnitz.e Abstract. We consier a variant
More informationA note on asymptotic formulae for one-dimensional network flow problems Carlos F. Daganzo and Karen R. Smilowitz
A note on asymptotic formulae for one-imensional network flow problems Carlos F. Daganzo an Karen R. Smilowitz (to appear in Annals of Operations Research) Abstract This note evelops asymptotic formulae
More informationStopping-Set Enumerator Approximations for Finite-Length Protograph LDPC Codes
Stopping-Set Enumerator Approximations for Finite-Length Protograph LDPC Coes Kaiann Fu an Achilleas Anastasopoulos Electrical Engineering an Computer Science Dept. University of Michigan, Ann Arbor, MI
More informationState-Space Model for a Multi-Machine System
State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal
More informationTHE GENUINE OMEGA-REGULAR UNITARY DUAL OF THE METAPLECTIC GROUP
THE GENUINE OMEGA-REGULAR UNITARY DUAL OF THE METAPLECTIC GROUP ALESSANDRA PANTANO, ANNEGRET PAUL, AND SUSANA A. SALAMANCA-RIBA Abstract. We classify all genuine unitary representations of the metaplectic
More informationLecture 5 January 16, 2013
UBC CPSC 536N: Sparse Approximations Winter 2013 Prof. Nick Harvey Lecture 5 January 16, 2013 Scribe: Samira Samadi 1 Combinatorial IPs 1.1 Mathematical programs { min c Linear Program (LP): T x s.t. a
More informationSeparation of Variables
Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical
More informationSYNCHRONOUS SEQUENTIAL CIRCUITS
CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents
More informationLecture #21. c T x Ax b. maximize subject to
COMPSCI 330: Design and Analysis of Algorithms 11/11/2014 Lecture #21 Lecturer: Debmalya Panigrahi Scribe: Samuel Haney 1 Overview In this lecture, we discuss linear programming. We first show that the
More informationA New Vulnerable Class of Exponents in RSA
A ew Vulnerable Class of Exponents in RSA Aberrahmane itaj Laboratoire e Mathématiues icolas Oresme Campus II, Boulevar u Maréchal Juin BP 586, 4032 Caen Ceex, France. nitaj@math.unicaen.fr http://www.math.unicaen.fr/~nitaj
More informationMath 1271 Solutions for Fall 2005 Final Exam
Math 7 Solutions for Fall 5 Final Eam ) Since the equation + y = e y cannot be rearrange algebraically in orer to write y as an eplicit function of, we must instea ifferentiate this relation implicitly
More informationApproximate Constraint Satisfaction Requires Large LP Relaxations
Approximate Constraint Satisfaction Requires Large LP Relaxations oah Fleming April 19, 2018 Linear programming is a very powerful tool for attacking optimization problems. Techniques such as the ellipsoi
More information7. Lecture notes on the ellipsoid algorithm
Massachusetts Institute of Technology Michel X. Goemans 18.433: Combinatorial Optimization 7. Lecture notes on the ellipsoid algorithm The simplex algorithm was the first algorithm proposed for linear
More informationA Path Planning Method Using Cubic Spiral with Curvature Constraint
A Path Planning Metho Using Cubic Spiral with Curvature Constraint Tzu-Chen Liang an Jing-Sin Liu Institute of Information Science 0, Acaemia Sinica, Nankang, Taipei 5, Taiwan, R.O.C., Email: hartree@iis.sinica.eu.tw
More informationLecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations
Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:
More informationThe continuity equation
Chapter 6 The continuity equation 61 The equation of continuity It is evient that in a certain region of space the matter entering it must be equal to the matter leaving it Let us consier an infinitesimal
More informationThe Approximability and Integrality Gap of Interval Stabbing and Independence Problems
CCCG 01, Charlottetown, P.E.I., August 8 10, 01 The Approximability an Integrality Gap of Interval Stabbing an Inepenence Problems Shalev Ben-Davi Elyot Grant Will Ma Malcolm Sharpe Abstract Motivate by
More informationarxiv: v1 [math.co] 15 Sep 2015
Circular coloring of signe graphs Yingli Kang, Eckhar Steffen arxiv:1509.04488v1 [math.co] 15 Sep 015 Abstract Let k, ( k) be two positive integers. We generalize the well stuie notions of (k, )-colorings
More informationPhysics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 3. 2 (x x ) 2 + (y y ) 2 + (z + z ) 2
Physics 505 Electricity an Magnetism Fall 003 Prof. G. Raithel Problem Set 3 Problem.7 5 Points a): Green s function: Using cartesian coorinates x = (x, y, z), it is G(x, x ) = 1 (x x ) + (y y ) + (z z
More informationProof of SPNs as Mixture of Trees
A Proof of SPNs as Mixture of Trees Theorem 1. If T is an inuce SPN from a complete an ecomposable SPN S, then T is a tree that is complete an ecomposable. Proof. Argue by contraiction that T is not a
More informationApplications of the Wronskian to ordinary linear differential equations
Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.
More informationQubit channels that achieve capacity with two states
Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March
More informationTutorial Test 5 2D welding robot
Tutorial Test 5 D weling robot Phys 70: Planar rigi boy ynamics The problem statement is appene at the en of the reference solution. June 19, 015 Begin: 10:00 am En: 11:30 am Duration: 90 min Solution.
More informationThe Impact of Collusion on the Price of Anarchy in Nonatomic and Discrete Network Games
The Impact of Collusion on the Price of Anarchy in Nonatomic an Discrete Network Games Tobias Harks Institute of Mathematics, Technical University Berlin, Germany harks@math.tu-berlin.e Abstract. Hayrapetyan,
More informationAdvanced Combinatorial Optimization September 22, Lecture 4
8.48 Advanced Combinatorial Optimization September 22, 2009 Lecturer: Michel X. Goemans Lecture 4 Scribe: Yufei Zhao In this lecture, we discuss some results on edge coloring and also introduce the notion
More informationThe chromatic number of graph powers
Combinatorics, Probability an Computing (19XX) 00, 000 000. c 19XX Cambrige University Press Printe in the Unite Kingom The chromatic number of graph powers N O G A A L O N 1 an B O J A N M O H A R 1 Department
More informationLATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION
The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische
More informationConvergence of Random Walks
Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of
More informationOnline Appendix for Trade Policy under Monopolistic Competition with Firm Selection
Online Appenix for Trae Policy uner Monopolistic Competition with Firm Selection Kyle Bagwell Stanfor University an NBER Seung Hoon Lee Georgia Institute of Technology September 6, 2018 In this Online
More informationThe Exact Form and General Integrating Factors
7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily
More informationUnit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule
Unit # - Families of Functions, Taylor Polynomials, l Hopital s Rule Some problems an solutions selecte or aapte from Hughes-Hallett Calculus. Critical Points. Consier the function f) = 54 +. b) a) Fin
More informationDuality of LPs and Applications
Lecture 6 Duality of LPs and Applications Last lecture we introduced duality of linear programs. We saw how to form duals, and proved both the weak and strong duality theorems. In this lecture we will
More informationLecture 11 October 7, 2013
CS 4: Advanced Algorithms Fall 03 Prof. Jelani Nelson Lecture October 7, 03 Scribe: David Ding Overview In the last lecture we talked about set cover: Sets S,..., S m {,..., n}. S has cost c S. Goal: Cover
More informationLinear First-Order Equations
5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)
More informationPractical Analysis of Key Recovery Attack against Search-LWE Problem
Practical Analysis of Key Recovery Attack against Search-LWE Problem IMI Cryptography Seminar 28 th June, 2016 Speaker* : Momonari Kuo Grauate School of Mathematics, Kyushu University * This work is a
More informationPhysics 5153 Classical Mechanics. The Virial Theorem and The Poisson Bracket-1
Physics 5153 Classical Mechanics The Virial Theorem an The Poisson Bracket 1 Introuction In this lecture we will consier two applications of the Hamiltonian. The first, the Virial Theorem, applies to systems
More informationAdvanced Combinatorial Optimization Updated April 29, Lecture 20. Lecturer: Michel X. Goemans Scribe: Claudio Telha (Nov 17, 2009)
18.438 Advanced Combinatorial Optimization Updated April 29, 2012 Lecture 20 Lecturer: Michel X. Goemans Scribe: Claudio Telha (Nov 17, 2009) Given a finite set V with n elements, a function f : 2 V Z
More informationCMSC 313 Preview Slides
CMSC 33 Preview Slies These are raft slies. The actual slies presente in lecture may be ifferent ue to last minute changes, scheule slippage,... UMBC, CMSC33, Richar Chang CMSC 33 Lecture
More informationA new proof of the sharpness of the phase transition for Bernoulli percolation on Z d
A new proof of the sharpness of the phase transition for Bernoulli percolation on Z Hugo Duminil-Copin an Vincent Tassion October 8, 205 Abstract We provie a new proof of the sharpness of the phase transition
More information6.854J / J Advanced Algorithms Fall 2008
MIT OpenCourseWare http://ocw.mit.edu 6.85J / 8.5J Advanced Algorithms Fall 008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.5/6.85 Advanced Algorithms
More informationGlobal Optimization for Algebraic Geometry Computing Runge Kutta Methods
Global Optimization for Algebraic Geometry Computing Runge Kutta Methos Ivan Martino 1 an Giuseppe Nicosia 2 1 Department of Mathematics, Stockholm University, Sween martino@math.su.se 2 Department of
More informationCHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold
CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the
More informationProblem set 2: Solutions Math 207B, Winter 2016
Problem set : Solutions Math 07B, Winter 016 1. A particle of mass m with position x(t) at time t has potential energy V ( x) an kinetic energy T = 1 m x t. The action of the particle over times t t 1
More informationLectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs
Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent
More informationu t v t v t c a u t b a v t u t v t b a
Nonlinear Dynamical Systems In orer to iscuss nonlinear ynamical systems, we must first consier linear ynamical systems. Linear ynamical systems are just systems of linear equations like we have been stuying
More informationAcute sets in Euclidean spaces
Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of
More informationarxiv: v1 [math.co] 13 Dec 2017
The List Linear Arboricity of Graphs arxiv:7.05006v [math.co] 3 Dec 07 Ringi Kim Department of Mathematical Sciences KAIST Daejeon South Korea 344 an Luke Postle Department of Combinatorics an Optimization
More informationNOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,
NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which
More informationAdvanced Combinatorial Optimization September 24, Lecture 5
18.438 Advanced Combinatorial Optimization September 24, 2009 Lecturer: Michel X. Goemans Lecture 5 Scribe: Yehua Wei In this lecture, we establish the connection between nowhere-zero (nwz) k-flow and
More informationPractical Analysis of Key Recovery Attack against Search-LWE Problem
Practical Analysis of Key Recovery Attack against Search-LWE Problem Royal Holloway an Kyushu University Workshop on Lattice-base cryptography 7 th September, 2016 Momonari Kuo Grauate School of Mathematics,
More informationn 1 conv(ai) 0. ( 8. 1 ) we get u1 = u2 = = ur. Hence the common value of all the Uj Tverberg's Tl1eorem
8.3 Tverberg's Tl1eorem 203 hence Uj E cone(aj ) Above we have erive L;=l 'Pi (uj ) = 0, an so by ( 8. 1 ) we get u1 = u2 = = ur. Hence the common value of all the Uj belongs to n;=l cone(aj ). It remains
More informationLecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012
CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration
More information19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control
19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior
More informationEntanglement is not very useful for estimating multiple phases
PHYSICAL REVIEW A 70, 032310 (2004) Entanglement is not very useful for estimating multiple phases Manuel A. Ballester* Department of Mathematics, University of Utrecht, Box 80010, 3508 TA Utrecht, The
More informationarxiv: v1 [math.co] 3 Apr 2019
Reconstructin phyloenetic tree from multipartite quartet system Hiroshi Hirai Yuni Iwamasa April 4, 2019 arxiv:1904.01914v1 [math.co] 3 Apr 2019 Abstract A phyloenetic tree is a raphical representation
More informationLecture 10: Logistic growth models #2
Lecture 1: Logistic growth moels #2 Fugo Takasu Dept. Information an Computer Sciences Nara Women s University takasu@ics.nara-wu.ac.jp 6 July 29 1 Analysis of the stochastic process of logistic growth
More informationLecturer: Shuchi Chawla Topic: Inapproximability Date: 4/27/2007
CS880: Approximations Algorithms Scribe: Tom Watson Lecturer: Shuchi Chawla Topic: Inapproximability Date: 4/27/2007 So far in this course, we have been proving upper bounds on the approximation factors
More informationDiagonalization of Matrices Dr. E. Jacobs
Diagonalization of Matrices Dr. E. Jacobs One of the very interesting lessons in this course is how certain algebraic techniques can be use to solve ifferential equations. The purpose of these notes is
More informationShortest-Elapsed-Time-First on a Multiprocessor
Shortest-Elapse-Time-First on a Multiprocessor Neal Barcelo, Sungjin Im 2, Benjamin Moseley 2, an Kirk Pruhs Department of Computer Science, University of Pittsburgh ncb30,kirk@cs.pitt.eu 2 Computer Science
More information12.11 Laplace s Equation in Cylindrical and
SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering
More informationOn combinatorial approaches to compressed sensing
On combinatorial approaches to compresse sensing Abolreza Abolhosseini Moghaam an Hayer Raha Department of Electrical an Computer Engineering, Michigan State University, East Lansing, MI, U.S. Emails:{abolhos,raha}@msu.eu
More informationThe derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)
Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)
More information