A Remark on Parabolic Index of Infinite

Similar documents
Prime Numbers and Irrational Numbers

Real Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi

JULIA SET OF THE FUNCTION zexp(z

REGULARITY OF POTENTIAL FUNCTIONS IN OPTIMAL TRANSPORTATION. Centre for Mathematics and Its Applications The Australian National University

MAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9

SUMS OF ULTRAFILTERS

Ideal boundary limit of discrete Dirichlet functions

ON SOME PROPERTIES OF ESSENTIAL DARBOUX RINGS OF REAL FUNCTIONS DEFINED ON TOPOLOGICAL SPACES

Lecture notes: Introduction to Partial Differential Equations

Mid Term-1 : Practice problems

PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS

BOUNDARY PROPERTIES OF FIRST-ORDER PARTIAL DERIVATIVES OF THE POISSON INTEGRAL FOR THE HALF-SPACE R + k+1. (k > 1)

NUMBERS. Michael E. Taylor

" W I T H M: A. L I G E T O ' W ^ P L D IST O ISTE -A-IsTD G H! A-I^IT Y IPO PL A.LI-i. :

ON THE PRODUCT OF SEPARABLE METRIC SPACES

MATH 173: Problem Set 5 Solutions

On the investigation of summable series *

A Proof of Convergence and an Error Bound for the Method of Bisection in R"

Groups. 3.1 Definition of a Group. Introduction. Definition 3.1 Group

MENGER'S THEOREM AND MATROIDS

The pure braid groups and the Milnor μ-invariants of links

0 Sets and Induction. Sets

A Generalized Sharp Whitney Theorem for Jets

Boundedly complete weak-cauchy basic sequences in Banach spaces with the PCP

ON A LEMMA OF BISHOP AND PHELPS

A CHARACTERIZATION OF COMPLETE LATTICES

Math 116 Practice for Exam 2

THE ELLIPTICITY PRINCIPLE FOR SELF-SIMILAR POTENTIAL FLOWS

Topological properties

Appendix B Convex analysis

ON AN INFINITE SET OF NON-LINEAR DIFFERENTIAL EQUATIONS By J. B. McLEOD (Oxford)

A BRANCHING LAW FOR THE SYMPLECTIC GROUPS

Commentationes Mathematicae Universitatis Carolinae

arxiv: v1 [math.oc] 21 Mar 2015

UNIQUENESS OF POSITIVE SOLUTIONS OF THE HEAT EQUATION

Lesson 3: Linear differential equations of the first order Solve each of the following differential equations by two methods.

Exercise Solutions to Functional Analysis

Extreme points of compact convex sets

DIAGONAL SUBMATRICES OF MATRIX MAPS

LECTURE 15: COMPLETENESS AND CONVEXITY

Introduction to Functional Analysis

AREA-BISECTING POLYGONAL PATHS. Warren Page New York City Technical College, CUNY

SOME FUNCTION CLASSES RELATED TO THE CLASS OF CONVEX FUNCTIONS

SOME ASPECTS ON CIRCLES AND HELICES IN A COMPLEX PROJECTIVE SPACE. Toshiaki Adachi* and Sadahiro Maeda

CONDITIONAL EXPECTATION IN AN OPERATOR ALGEBRA

On a certain type of matrices with an application to experimental design

Topics in Harmonic Analysis Lecture 6: Pseudodifferential calculus and almost orthogonality

CLASSIFICATION AND PRINCIPLE OF SUPERPOSITION FOR SECOND ORDER LINEAR PDE

Math 172 Problem Set 5 Solutions

Homework I, Solutions

Hilbert s Metric and Gromov Hyperbolicity

MATH 31BH Homework 1 Solutions

Math 222 Spring 2013 Exam 3 Review Problem Answers

TRANSLATION-INVARIANT FUNCTION ALGEBRAS ON COMPACT GROUPS

FIXED POINT THEOREMS FOR POINT-TO-SET MAPPINGS AND THE SET OF FIXED POINTS

Math 31CH - Spring Final Exam

APPROXIMATE ISOMETRIES ON FINITE-DIMENSIONAL NORMED SPACES

A local Crank-Nicolson method for solving the heat equation. Abdurishit ABUDUWALI, Michio SAKAKIHARA and Hiroshi NIKI

Smooth Dependence of Solutions of Differential Equations on Initial Data: A Simple Proof*

2) Let X be a compact space. Prove that the space C(X) of continuous real-valued functions is a complete metric space.

RANDOM FIBONACCI-TYPE SEQUENCES

Sec. 14.3: Partial Derivatives. All of the following are ways of representing the derivative. y dx

F O R M U L A S F O R CONVOLUTION F I B O N A C C I NUMBERS AND P O L Y N O M I A L S

ON SYMMETRIC SETS OF UNIMODULAR SYMMETRIC MATRICES

ON THE ERDOS-STONE THEOREM

UNIVERSAL DERIVED EQUIVALENCES OF POSETS

0.1 Pointwise Convergence

Introduction to Topology

ON THE RANGE OF A DERIVATION

ARCS IN FINITE PROJECTIVE SPACES. Basic objects and definitions

A generalization of Magnus' theorem. Osaka Journal of Mathematics. 14(2) P.403-P.409

Complex Variables. Chapter 2. Analytic Functions Section Harmonic Functions Proofs of Theorems. March 19, 2017

GAUSSIAN MEASURES ON 1.1 BOREL MEASURES ON HILBERT SPACES CHAPTER 1

2. A die is rolled 3 times, the probability of getting a number larger than the previous number each time is

ALGEBRAIC GEOMETRY (NMAG401) Contents. 2. Polynomial and rational maps 9 3. Hilbert s Nullstellensatz and consequences 23 References 30

Notes on Continued Fractions for Math 4400

CLASS NOTES FOR APRIL 14, 2000

FUNCTION BASES FOR TOPOLOGICAL VECTOR SPACES. Yılmaz Yılmaz

NOTES ON SIMPLE NUMBER THEORY

Introduction and Preliminaries

Linear Normed Spaces (cont.) Inner Product Spaces

ON THE CAUCHY EQUATION ON SPHERES

Banach Spaces II: Elementary Banach Space Theory

SYMMETRICOMPLETIONS AND PRODUCTS OF SYMMETRIC MATRICES

Lecture Notes in Advanced Calculus 1 (80315) Raz Kupferman Institute of Mathematics The Hebrew University

Taylor and Laurent Series

We will begin our study of topology from a set-theoretic point of view. As the subject

Hyperbolic Nonwandering Sets on Two-Dimensional Manifolds 1

MATH 54 - TOPOLOGY SUMMER 2015 FINAL EXAMINATION. Problem 1

A note on some approximation theorems in measure theory

ON A DISTANCE DEFINED BY THE LENGTH SPECTRUM ON TEICHMÜLLER SPACE

2.3 Linear Equations 69

POSITIVE SELF ADJOINT EXTENSIONS OF POSITIVE SYMMETRIC OPERATORS TSUYOSHI ANDO AND KATSUYOSHI NISHIO. (Received June 30, 1969)

= ϕ r cos θ. 0 cos ξ sin ξ and sin ξ cos ξ. sin ξ 0 cos ξ

NATIONAL BOARD FOR HIGHER MATHEMATICS. Research Scholarships Screening Test. Saturday, February 2, Time Allowed: Two Hours Maximum Marks: 40

Continuous Random Variables

Monochromatic Forests of Finite Subsets of N

MATH34032 Mid-term Test 10.00am 10.50am, 26th March 2010 Answer all six question [20% of the total mark for this course]

A Generalization of Kukri's Theorem for an Infinite Game

MATH443 PARTIAL DIFFERENTIAL EQUATIONS Second Midterm Exam-Solutions. December 6, 2017, Wednesday 10:40-12:30, SA-Z02

Transcription:

HIROSHIMA MATH. J. 7 (1977), 147-152 A Remark on Parabolic Index of Infinite Networks Fumi-Yuki MAEDA (Received September 16, 1976) In the preceding paper [1], M. Yamasaki introduced the notion of parabolic index of infinite networks. He proposed (orally) a problem to determine the parabolic index of the infinite network N d formed by the lattice points and the segments parallel to coordinate axes in the d-dimensional euclidean space. The purpose of the present paper is to show that the parabolic index of N d is equal to the dimension d. This is a discrete analogue of the well-known fact that infί Jgrad/ *dx = 0 if and only if p^d, where the infimum is taken over all C 1 -functions / on R d with compact support such that/^ 1 on a fixed ball in R d. For notation and terminologies, we mainly follow [1]. 1. Description of the network Let R d be the rf-dimensional euclidean space (d^l). Let X (d) be the set of all lattice points, i.e., χ(d) = <* (Z: the set of integers). Let e l9 e d be the standard base of R d, i.e., the /c-th component of e j is 1 for k=j and 0 for k+j. For α, ber d 9 let [α, b~\ denote the directed line segment from a to b. For each j (=1,..., d) 9 set Sft = {[x, x + ejl; x = (v l9 v d )ex«\ Vj ^ 0}, and S%L = {[x, x-^]; x = (v lf..., v d )ex^\ Vj 0} We define Y<» by For xex< d > and y = [x ί9 x 2 ]e 7< d >, let

148 Fumi-Yuki MAEDA 1, if x 2 = x, -1, if x^x, 0, if Xj Φ x and x 2 Φ x. With r(y) = l, N d = {X (d \ Y (d) 9 What we shall prove is K, r} is an infinite network in the sense of [1]. THEOREM. lnάn d =d. Here lnάn d is the parabolic index of N d (see [1, 5]). The case d = l is proved in [1, Example 4.1]. The proof for d^2 consists of two parts: (I) If p^d 9 then N d is of parabolic type of order p\ (II) If 1 <p<d, then N d is of hyperbolic type of order p. For simplicity, we shall omit the superscript (d) in the notation. For x = (v 1?..., v d )εx, we write x = ( v 1,..., v d ) and x =max y v j. For y = [x ί9 x 2 ] e 7, the point x^ will be denoted by a(y)\ if y ε S J9 then the index j will be denoted 2. Proof of (I) Let X n ={xex', \\x\\ ^n}, n = 0, 1,... and Y n = {[^ι? ^]e7; x 1? x e^π}, 2 n = 1, 2,... Then {<X n, Y n >} is an exhaustion of N d. It is elementary to see that -*, n = 1,2,... (Here, Card stands for the cadinal.) Hence, if we put Z n =7 π Y n, l (7 0 = 0), then CardZ M = Card Y n - Card Y n _ 1 ^ \ n = 1,2,... Since r(y)=! 9 μ ( p) n = Σ roo 1 -*- CardZ π ^ yez n Hence, if p^.d and 1/p +1/^ = 1, then -ι, n = 1, 2,.... Σ π=l = +00,

A Remark on Parabolic Index of Infinite Networks 149 since (d- l)(l-g)^ -1. Therefore, by [1, Corollary 1 to Theorem 4.1], N d is of parabolic type of order p if p Ξ> d. 3. Proof of (II) We shall prove (II) in several steps. Let 0> be the set of all permutations of {!,...,</} and for x = (v l9..., v d ) and πe^, let π*x = (v π(1),..., v π(d) ). (i) For y,y'ey 9 if there is πe0> such that π* α(^) = α(/) and j(y)=* π(y(/)), then we say that y and / are equivalent and write y~y'. Obviously, this is an equivalence relation in Y. Now we put and Observe that for x* = (μ ί9 μ d )e X*, x* + ^ e^* (resp. x*-ej ex*) if and only if j = min {k\ μ k = μ y } (resp. μ y ^ 0 and 7 = max {fe; μ fc = μj}). Using this fact, we can easily see that y* is a set of representatives with respect to the equivalence relation ~, i.e., for every ye 7, there is exactly one y* e Y* such that.y*~.y. (ii) In order to construct a flow from {0} to oo, we consider the following values defined inductively : d) ι;7 + l) = 2-1 7'(</-7')~ 1 {(2n-l)F(n; j)-(2n + iy- d }, j = 1, 2,..., d-1, n = 1, 2,... In a closed form, F(n; 7) is expressed as which is verified by induction on j. Observing that / d-\ \ < (d-j we obtain (2) / (n;y)g(2n-l)-' i, y = 1,,.., d; n = 1, 2,.

150 Fumi-Yuki MAEDA (iii) Given x* = (μ 1,,.., μ d )ex*, let /c(x*) denote the largest integer k such that μ k = μ l. We define a function w on Y as follows: (a) If y = [x*, x' + eje Y* and x* = ( μι,..., μ d ), then (b) If y = [x*, x* + e, ]ey* with7>l and x* = (μ 1,..., μ d ), then w(j ) = (2dr 1 (2μ j +l)f(μ ί ' y /c(x*)+l) (c) If y e 7-7*, then \v(y) = w(j;*) for y* e 7 * such that y* ~ >>. Now we shall prove that w is a flow (see [1, 4]) from {0} to oo with strength /(w)=l. (iii-1) Every ye Y(0) is equivalent to y* = [Q, e^ey* (see [1, (1.3)] for y(x)). Therefore, w(y) = w(y*) = (2ί/)- 1 for all y e y(0), and hence (iii-2) Let x = (v lv.., v d )e X and x^o. Choose x* = (μ l5..., μ^ex* such that π* x =x* for some πe^9. For each 7, let us compute Σyes^ ^( If Vj > 0 (resp. v 7 < 0), then y(x) n Sj = {[x, x + ej, [x-^, x]} (resp. = {[x, x-e y ], [x + e,, x]}). For ^ι = [x, x + βj] (resp. [x, x ej]\ choose π so that π'hλ = min{/c; v π(k) = v 7 }. Then J* = [x*, x* + ^m] (m = π~ 1 (7)) belongs to y* and is equivalent to y^. Since μ m = l v yl an d m = l if and only if \Vj\=μ ί9 (2d)-H2μ 1 + l) 1 - d, if \Vj\=μ i 9 (2d)- 1 (2 v y + l)f( μι /c(x*)+ 1), if v y < μ x. For y 2 = [* "~ ^» χ ] (resp. [x + e j9 x]), choose π so that π'hλ = max{/c; v π(k) = IvJ}. Then 3>2 = [**-em> x *l ( m = π~ 1 (Λ) belongs to y* and is equivalent to >' 2. The m-th component of x* e m is equal to \Vj\- 1; m = l if and only if ^^1=^! and /c(χ*) = 1. Furthermore, f /c(x*)-l, if v, = μi and fc(x*) > 1, /c(**-o = 1 /c(x*), if \vj\<μi.

A Remark on Parabolic Index of Infinite Networks 151 Hence (2μ-\γ-* =(2d)- ί (2μ 1 -ί)f(μ l ; fc(x*)), W (y 2 ) = if vy = μι and k(x*) = 1, (2dΓ 1 (2μ 1 - l)f(μ ί fc(x*)), if v,. = μ, and fc(x ) > 1, Therefore, in case v,-^0, using (1) we have (3) (2</)-K2 v, - l)f(μ, fc(x*) + 1), if \ Vj \ < μ,. if If v, =0, then ;fc(x*)+l), if \Vj\< μι. Y(x) n Sy = {[x, x + ej ], [x, x- and by an argument similar to the above, we see that both JΊ = [X, x + e y ] and y2 = \x,*-ej\ are equivalent to y* = [x*, x* + e m ] e 7*. Since Vy=0, m?έl. Hence, in case v y =0, we have (4) Σ K(x, y)w(y) = - w^) - w(); 2 ) = - 2w(y*) = - d~ l F(μ tfc(x*) + 1). jiesj Combining (3) and (4), we have in any case ti ;*(**) +!). if I vj I -ML - -F( μi k(x*) + I), if I Vj I <μ,. Since Card {;; v j - =μ 1 } = fc(x*), Σ K(x, j)w(y) = Σ Σ jiey j=l yesj κ(χ, -{d-k(x*)}d- l F( μί ;k(x*)+l) = 0. Therefore, w is a flow from {0} to oo.

152 Fumi-Yuki MAEDA (iv) Finally, we show that if i<p<d and 1/p + l/g = l, then Σ w(y)«< If y~y*εy* and a(y*) = (μ l9 μ d ) 9 and μ'^1, then then μ 1 = α(y)... Hence if j(y*) and if j(y*)> 1, then μ j(y^μ^ 1, so that by virtue of (2), Now let T H = {yey; \\a(y)\\ =n}, n = 0, 1,.... Then y=\js B0 7i- For each x e X with x = π, there are at most 2d elements y in Γsuch that a(y) = x. Hence, Card Γ 0 = 2d and Card T n g 2c/Card(X M -X n _ 1 ), /ι = 1, 2,.... On the other hand, Card X n = (2n + l) d. Hence CardT, ^ ^(Σn + l)^1, n = 1, 2,.... Therefore Σ w(y)^ = Σ Σ yef n=0 3>eΓ n woo* g 2d(2d)-«+ Σ 4ί/ 2 (2n + l)''- 1 (2c/)-«(2n-l)' 1 -''>«< +00, «=1 since p < d implies d 1 + (1 d)q < 1. (v) Now the statement of (II) follows from [1, Theorem 4.3]. Reference [ 1 ] M. Yamasaki, Parabolic and hyperbolic infinite networks, this journal., 135-146. Department of Mathematics, Faculty of Science, Hiroshima University