DOCSLIB.ORG

Smoothness of Projections, Bernoulli Convolutions, and Dimensions Of

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Smoothness of Projections, Bernoulli Convolutions, and Dimensions Of SMOOTHNESS OF PROJECTIONS, BERNOULLI CONVOLUTIONS, AND THE DIMENSION OF EXCEPTIONS YUVAL PERES AND WILHELM SCHLAG n Abstract. Erd˝os (1939, 1940) studied the distribution ν of the random series ∞ λ ,andshowedthat λ 0 ± ν is singular for infinitely many λ (1/2, 1), and absolutely continuous for a.e. λ in a small interval λ ∈ P (1 δ, 1). Solomyak (1995) proved a conjecture made by Garsia (1962) that ν is absolutely continuous − λ for a.e. λ (1/2, 1). In order to sharpen this result, we have developed a general method that can be used ∈ to estimate the Hausdorffdimension of exceptional parameters in several contexts. In particular, we prove: For any λ0 > 1/2, the set of λ [λ0, 1) such that ν is singular has Hausdorffdimension strictly less than 1. • ∈ λ For any Borel set A d with Hausdorffdimension dim A>(d +1)/2, there are points x A such that • ⊂ R ∈ the pinned distance set x y : y A has positive Lebesgue measure. Moreover, the set of x where this {| − | ∈ } fails has Hausdorffdimension at most d +1 dim A. − Let denote the middle-α Cantor set for α =1 2λ and let K be any compact set. Peres and • Kλ − ⊂ R Solomyak (1998) showed that for a.e. λ (λ0, 1/2) such that dim K +dim > 1, the sum K + has ∈ Kλ Kλ positive length; we show that the set of exceptional λ in this statement has Hausdorffdimension at most 2 dim K dim . − − Kλ0 For any Borel set E d with dim E>2, almost all orthogonal projections of E onto lines through • ⊂ R the origin have nonempty interior, and the exceptional set of lines where this fails has dimension at most d +1 dim E. − d If µ is a Borel probability measure on R with correlation dimension greater than m +2γ,thenfora • 1 d m “prevalent” set of C maps f : R R (in the sense described by Hunt, Sauer and Yorke (1992)), the → 2 m image of µ under f has a density with at least γ fractional derivatives in L (R ). 1. Introduction n The distribution νλ of the random series 0∞ λ , where the signs are chosen independently with proba- 1 ± bility 2 , has been studied by many authors since the two seminal papers by Erd˝osin 1939 and 1940. It is 1 1 immediate that νλ is singular for λ< 2 . In [6], Erd˝osshowed that νλ is singular for infinitely many λ ( 2 , 1), 1 ∈ namely those λ such that λ− is a Pisot number, and in [7] he proved that νλ is absolutely continuous for a.e. λ (1 δ, 1) where δ<0.01. It had been observed before by Jessen and Wintner [21] that νλ is either absolutely∈ continuous− or singular with respect to Lebesgue measure for any choice of λ. Works of Alexander and Yorke [2], Przytycki and Urba´nski [37], and Ledrappier [27] showed the importance of these distributions in several problems in dynamical systems. Solomyak [39] proved a conjecture made by Garsia in 1962, that νλ 2 is absolutely continuous for a.e. λ (1/2, 1); in fact, he showed that νλ has density in L for a.e. λ (1/2, 1). Peres and Solomyak [34] then gave∈ a simpler proof of this. A survey of the results obtained on∈ Bernoulli convolutions from the 1930’s to 1999 is presented in [33]. 2 In the present paper, we show that the density of νλ has a fractional derivative in L for a.e. λ (1/2, 1), and obtain a bound on the integrated Sobolev norm. We then use this bound to establish that∈ for any closed interval I (1/2, 1], the set of λ I such that νλ is singular, has Hausdorffdimension less than 1 (Theorem 5.4 and⊂ Corollary 5.6). In order∈ to prove these results, we were led to develop a general method, which can be applied to improve previous results on Hausdorffdimensions of sums of Cantor sets, distance sets, 1991 Mathematics Subject Classification. Primary 42B25; Secondary 28A78. Y. Peres was partly supported by NSF grant DMS–9404391. W. Schlag was supported by a NSF postdoctoral fellowship at the Mathematical Sciences Research Institute, Berkeley. 1 2 YUVALPERESANDWILHELMSCHLAG and self-similar sets with deleted digits. (An exposition of our method for the case of Bernoulli convolutions is in [33]). Heuristically, the measures νλ may be viewed as nonlinear projections of the uniform measure on sequence space. Indeed, the analysis of νλ in [39] and [34] employed techniques developed by Kaufman [23] and Mattilla [30] to study orthogonal projections of sets and measures in Euclidean space. The following (informally stated) principles were first discovered by Marstrand [28], Kaufman [23, 24] and Mattila [29, 30] in the study of orthogonal projections, and then extended to a variety of other settings by Falconer [12], Hu and Taylor [16], Pollicott and Simon [36], Solomyak [39, 40, 41], Peres and Solomyak [34, 35] and Sauer and Yorke [38]. If an m dimensional measure is “projected” to m dimensional space, then “typically” its di- • mension− is preserved. If an m + dimensional measure is “projected” to m dimensional space, then “typically” the • projected measure is absolutely continuous, with a density in L2. In making these principles precise, the appropriate notion of dimension of measures must be used (Correlation or information dimension, but not Minkowski or packing dimension; see Jarvenp¨a¨a[20] and [38]), and the parametrized family of generalized projections considered must be sufficiently rich (at least m dimensional). A more delicate requirement is a certain “transversality condition” (e.g., Lemma 3.11 in [31]). For Bernoulli convolutions and other self-similar measures, this condition involves bounds on the double zeros of certain power series, and it was first made explicit by Pollicott and Simon [36]. Transversality is crucial in the works of Solomyak [39, 40, 41], Peres and Solomyak [34, 35], and in the present paper. The general principles that underly our work can be informally stated as follows: If an m dimensional measure µ is “projected” to an m dimensional space, then the set of • parameters− where the projection of µ has lower dimension than µ itself, has “codimension” at least . If an m + dimensional measure is “projected” to m dimensional space, then “typically” the • projected measure has a density with a fractional derivative of order /2inL2, and the set of parameters where the projected measure is singular has “codimension” at least . The notion of Sobolev dimension of a measure, defined in (2.3) below, yields a unification of these two princi- ples. For orthogonal projections, these strengthened principles have been stated precisely, and established as theorems, by Kaufman [24], Falconer [9] and Mattila [29], except that they did not consider fractional deriva- tives. Their proofs are based on averaging with respect to an appropriate Frostman measure on parameter space. In the setting of Bernoulli convolutions, this averaging approach is not powerful enough to establish the last principle, so we were forced to develop a different technique. Our methods apply to several concrete problems, which we now describe. Throughout the paper, dim (without subscripts) will mean Hausdorffdimension. Orthogonal projections. To motivate the general formulations, we start by clarifying the impor- • tant results of Falconer [9] on exceptional directions for projections in Rd (see Sections 2 and 6). As a corollary, we find that for any Borel set E Rd with dim E>2 and for a.e. direction θ in the d 1 ⊂ sphere S − , the orthogonal projection projθ(E) of E to the line through 0 and θ, has nonempty interior. More precisely (see corollary 6.2), d 1 dim θ S − :proj(E) has empty interior d +1 dim E. { ∈ θ }≤ − n Symmetric Bernoulli Convolutions. Let νλ be the distribution of the random series n∞=0 λ , • n ± so νλ has the Fourier transform νλ(ξ)= ∞ cos(λ ξ). Here we sharpen the result of Solomyak [39] n=0 that νλ is absolutely continuous for a.e. λ (1/2, 1), by showing that the 2,γ–Sobolev norm satisfies ∈ ∞ ν 2 = ν (ξ) 2 ξ 2γ dξ< λ2,γ | λ | | | ∞ −∞ SMOOTHNESS OF PROJECTIONS 3 for a.e. λ<0.649 such that λ1+2γ > 1/2. Moreover, for some constant C>0, and all small >0, we have dim λ (1/2+, 1) : ν is singular < 1 C. ∈ λ − p n Asymmetric Bernoulli Convolutions. Let νλ be the distribution of the sum n∞=0 λ • where the signs are chosen randomly and independently with probabilities (p, 1 p). Peres± and p p 1 p − p Solomyak [35] showed that ν is absolutely continuous for a.e. λ (p (1 p) − , 1), but ν has a λ ∈ − λ density in L2 for a.e. λ (p2 +(1 p)2, 1), and not for any smaller λ. The Pisot numbers still ∈ − p provide infinitely many examples of singular νλ. In the present paper, we show that ∞ νp(ξ) 2 ξ 2γ dξ< | λ | | | ∞ −∞ for a.e. λ<0.649 such that λ1+2γ >p2 +(1 p)2. Moreover, if p (1/3, 2/3), then for some constant C>0, and all >0, − ∈ dim λ (p2 +(1 p)2 + , 1) : νp L2 < 1 C, ∈ − λ ∈ − and p 1 p p dim λ (p (1 p) − + , 1) : ν is singular < 1 C. ∈ − λ − d d Intersections of sets with spheres Suppose E R is a Borel set with d 2. Let S0 R be • ⊂ ≥ ⊂ a strictly convex, closed C∞–hypersurface surrounding the origin. Then d dim x R :(x + rS0) E = for a.e.
Load more

Recommended publications
  • Perfect Filtering and Double Disjointness
    ANNALES DE L’I. H. P., SECTION B HILLEL FURSTENBERG YUVAL PERES BENJAMIN WEISS Perfect filtering and double disjointness Annales de l’I. H. P., section B, tome 31, no 3 (1995), p. 453-465 <http://www.numdam.org/item?id=AIHPB_1995__31_3_453_0> © Gauthier-Villars, 1995, tous droits réservés. L’accès aux archives de la revue « Annales de l’I. H. P., section B » (http://www.elsevier.com/locate/anihpb) implique l’accord avec les condi- tions générales d’utilisation (http://www.numdam.org/conditions). Toute uti- lisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Henri Poincaré, Vol. 31, n° 3, 1995, p. 453-465. Probabilités et Statistiques Perfect filtering and double disjointness Hillel FURSTENBERG, Yuval PERES (*) and Benjamin WEISS Institute of Mathematics, the Hebrew University, Jerusalem. ABSTRACT. - Suppose a stationary process ~ Un ~ is used to select from several stationary processes, i.e., if Un = i then we observe Yn which is the n’th variable in the i’th process. when can we recover the selecting sequence ~ Un ~ from the output sequence ~Yn ~ ? RÉSUMÉ. - Soit ~ Un ~ un processus stationnaire utilise pour la selection de plusieurs processus stationnaires, c’ est-a-dire si Un = i alors on observe Yn qui est le n-ième variable dans le i-ième processus. Quand peut-on reconstruire ~ Un ~ à partir de ~ Yn ~ ? 1. INTRODUCTION Suppose a discrete-time stationary stochastic signal ~ Un ~, taking integer values, is transmitted over a noisy channel.
    [Show full text]
  • Russell David Lyons
    Russell David Lyons Education Case Western Reserve University, Cleveland, OH B.A. summa cum laude with departmental honors, May 1979, Mathematics University of Michigan, Ann Arbor, MI Ph.D., August 1983, Mathematics Sumner Myers Award for best thesis in mathematics Specialization: Harmonic Analysis Thesis: A Characterization of Measures Whose Fourier-Stieltjes Transforms Vanish at Infinity Thesis Advisers: Hugh L. Montgomery, Allen L. Shields Employment Indiana University, Bloomington, IN: James H. Rudy Professor of Mathematics, 2014{present. Indiana University, Bloomington, IN: Adjunct Professor of Statistics, 2006{present. Indiana University, Bloomington, IN: Professor of Mathematics, 1994{2014. Georgia Institute of Technology, Atlanta, GA: Professor of Mathematics, 2000{2003. Indiana University, Bloomington, IN: Associate Professor of Mathematics, 1990{94. Stanford University, Stanford, CA: Assistant Professor of Mathematics, 1985{90. Universit´ede Paris-Sud, Orsay, France: Assistant Associ´e,half-time, 1984{85. Sperry Research Center, Sudbury, MA: Researcher, summers 1976, 1979. Hampshire College Summer Studies in Mathematics, Amherst, MA: Teaching staff, summers 1977, 1978. Visiting Research Positions University of Calif., Berkeley: Visiting Miller Research Professor, Spring 2001. Microsoft Research: Visiting Researcher, Jan.{Mar. 2000, May{June 2004, July 2006, Jan.{June 2007, July 2008{June 2009, Sep.{Dec. 2010, Aug.{Oct. 2011, July{Oct. 2012, May{July 2013, Jun.{Oct. 2014, Jun.{Aug. 2015, Jun.{Aug. 2016, Jun.{Aug. 2017, Jun.{Aug. 2018. Weizmann Institute of Science, Rehovot, Israel: Rosi and Max Varon Visiting Professor, Fall 1997. Institute for Advanced Studies, Hebrew University of Jerusalem, Israel: Winston Fellow, 1996{97. Universit´ede Lyon, France: Visiting Professor, May 1996. University of Wisconsin, Madison, WI: Visiting Associate Professor, Winter 1994.
    [Show full text]
  • Affine Embeddings of Cantor Sets on the Line Arxiv:1607.02849V3
    Affine Embeddings of Cantor Sets on the Line Amir Algom August 5, 2021 Abstract Let s 2 (0; 1), and let F ⊂ R be a self similar set such that 0 < dimH F ≤ s . We prove that there exists δ = δ(s) > 0 such that if F admits an affine embedding into a homogeneous self similar set E and 0 ≤ dimH E − dimH F < δ then (under some mild conditions on E and F ) the contraction ratios of E and F are logarithmically commensurable. This provides more evidence for Conjecture 1.2 of Feng et al.(2014), that states that these contraction ratios are logarithmically commensurable whenever F admits an affine embedding into E (under some mild conditions). Our method is a combination of an argument based on the approach of Feng et al.(2014) with a new result by Hochman(2016), which is related to the increase of entropy of measures under convolutions. 1 Introduction Let A; B ⊂ R. We say that A can be affinely embedded into B if there exists an affine map g : R ! R; g(x) = γ · x + t for γ 6= 0; t 2 R, such that g(A) ⊆ B. The motivating problem of this paper to show that if A and B are two Cantor sets and A can be affinely embedded into B, then the there should be some arithmetic dependence between the scales appearing in the multiscale structures of A and B. This phenomenon is known to occur e.g. when A and B are two self similar sets satisfying the strong separation condition that are Lipschitz equivalent, see Falconer and Marsh(1992).
    [Show full text]
  • Characterization of Cutoff for Reversible Markov Chains
    Characterization of cutoff for reversible Markov chains Riddhipratim Basu ∗ Jonathan Hermon y Yuval Peres z Abstract A sequence of Markov chains is said to exhibit (total variation) cutoff if the conver- gence to stationarity in total variation distance is abrupt. We consider reversible lazy chains. We prove a necessary and sufficient condition for the occurrence of the cutoff phenomena in terms of concentration of hitting time of \worst" (in some sense) sets of stationary measure at least α, for some α (0; 1). 2 We also give general bounds on the total variation distance of a reversible chain at time t in terms of the probability that some \worst" set of stationary measure at least α was not hit by time t. As an application of our techniques we show that a sequence of lazy Markov chains on finite trees exhibits a cutoff iff the product of their spectral gaps and their (lazy) mixing-times tends to . 1 Keywords: Cutoff, mixing-time, finite reversible Markov chains, hitting times, trees, maximal inequality. arXiv:1409.3250v4 [math.PR] 18 Feb 2015 ∗Department of Statistics, UC Berkeley, California, USA. E-mail: [email protected]. Supported by UC Berkeley Graduate Fellowship. yDepartment of Statistics, UC Berkeley, USA. E-mail: [email protected]. zMicrosoft Research, Redmond, Washington, USA. E-mail: [email protected]. 1 1 Introduction In many randomized algorithms, the mixing-time of an underlying Markov chain is the main component of the running-time (see [21]). We obtain a tight bound on tmix() (up to an absolute constant independent of ) for lazy reversible Markov chains in terms of hitting times of large sets (Proposition 1.7,(1.6)).
    [Show full text]
  • Amber L. Puha, Phd June 2021 Department of Mathematics Craven Hall 6130 California State University San Marcos Office Phone: 1-760-750-4201 333 S
    Amber L. Puha, PhD June 2021 Department of Mathematics Craven Hall 6130 California State University San Marcos Office Phone: 1-760-750-4201 333 S. Twin Oaks Valley Road Department Phone: 1-760-750-8059 San Marcos, CA 92096-0001 https://faculty.csusm.edu/apuha/ [email protected] Appointments 2010{present, Professor, Department of Mathematics, CSU San Marcos 2020-2021, Sabbatical Leave of Absence, Research Associate and Teaching Visitor Department of Mathematics, UCSD 2013-2014, Sabbatical Leave of Absence, Research Associate and Teaching Visitor Department of Mathematics, UCSD 2010-2011, Professional Leave of Absence 2009{2011, Associate Director, Institute for Pure and Applied Mathematics (IPAM), UCLA 2004-2010, Associate Professor, Department of Mathematics, CSU San Marcos 2009-2010, Professional Leave of Absence 2005-2006, Sabbatical Leave of Absence, Research Associate and Teaching Visitor, Department of Mathematics, UCSD 1999-2004, Assistant Professor, Department of Mathematics, CSU San Marcos 2000-2001 & Spring 2002, Professional Leave of Absence, National Science Foundation Mathematical Sciences Postdoctoral Fellow Research Interests Probability Theory and Stochastic Processes, with emphasis on Stochastic Networks Professional Awards 2021-2024, PI, National Science Foundation Single-Investigator Award, DMS-2054505, $232,433 2020{2021, CSUSM Research, Scholarship and Creative Activity (RSCA) Grant, $7,200 2019{2020, CSUSM Research, Scholarship and Creative Activity (RSCA) Grant, $2,000 2019, National Scholastic Surfing Association,
    [Show full text]
  • Front Matter
    Cambridge University Press 978-1-107-13411-9 — Fractals in Probability and Analysis Christopher J. Bishop , Yuval Peres Frontmatter More Information CAMBRIDGE STUDIES IN ADVANCED MATHEMATICS 162 Editorial Board B. BOLLOBAS,´ W. FULTON, F. KIRWAN, P. SARNAK, B. SIMON, B. TOTARO FRACTALS IN PROBABILITY AND ANALYSIS A mathematically rigorous introduction to fractals which emphasizes examples and fundamental ideas. Building up from basic techniques of geometric measure theory and probability, central topics such as Hausdorff dimension, self-similar sets and Brownian motion are introduced, as are more specialized topics, including Kakeya sets, capacity, percolation on trees and the Traveling Salesman Theorem. The broad range of techniques presented enables key ideas to be highlighted, without the distraction of excessive technicalities. The authors incorporate some novel proofs which are simpler than those available elsewhere. Where possible, chapters are designed to be read independently so the book can be used to teach a variety of courses, with the clear structure offering students an accessible route into the topic. Christopher J. Bishop is a professor in the Department of Mathematics at Stony Brook University. He has made contributions to the theory of function algebras, Kleinian groups, harmonic measure, conformal and quasiconformal mapping, holomorphic dynamics and computational geometry. Yuval Peres is a Principal Researcher at Microsoft Research in Redmond, WA. He is particularly known for his research in topics such as fractals and Hausdorff measure, random walks, Brownian motion, percolation and Markov chain mixing times. In 2016 he was elected to the National Academy of Science. © in this web service Cambridge University Press www.cambridge.org Cambridge University Press 978-1-107-13411-9 — Fractals in Probability and Analysis Christopher J.
    [Show full text]
  • CHRISTOPHER J. BISHOP Department of Mathematics Stony Brook University Stony Brook, NY 11794-3651
    CHRISTOPHER J. BISHOP Department of Mathematics Stony Brook University Stony Brook, NY 11794-3651 RESEARCH INTERESTS Real and complex analysis, geometric function theory, conformal dynamics, probability theory, numerical analysis, analysis on fractals, quasiconformal geometry, computational geometry. Some of my more particular interests have included: potential theory, fractal properties of harmonic measure, geometric properties of Brownian motion and other random processes, al- gebras generated by harmonic and holomorphic functions, geometry of hyperbolic manifolds and their covering groups, numerical computation of conformal mappings, multipole methods, optimal meshing algorithms, nonobtuse triangulation, quadrilateral meshing, iteration of entire functions and dimension distorting properties of quasiconformal maps. I program in C, Mathe- matica and Matlab as part of my investigations in these areas, and teach a class on experimental aspects of mathematics. PROFESSIONAL EXPERIENCE Sept. 1997 to present: Professor at Stony Brook University. Sept. 1992 to Aug. 1997: Assoc. professor at Stony Brook. Sept. 1991 to Aug. 1992: Asst. professor at Stony Brook. Sept. 1988 to Aug. 1991: Hedrick Asst. professor at UCLA. Sept. 1987 to Aug. 1988: NSF postdoc at MSRI, Berkeley. EDUCATION Cambridge University, Master of Advanced Study (MASt), 2011. University of Chicago, Mathematics, Ph. D., 1987, Advisor Peter W. Jones. Visiting graduate student and programmer, Dept. of Mathematics, Yale University, 1985-1987. University of Chicago, Mathematics, Master of Science, 1984. Cambridge University, Certificate of Advanced Study (Part III of Math. Tripos), 1983. Michigan State University, Mathematics, Bachelor of Science, 1982. PH.D. STUDENTS Zsuzsanna Gonye, Ph. D. 2001, Geodesics in hyperbolic manifolds, Assoc. Professor, University of West Hungary Karyn Lundberg, Ph. D. 2005, Boundary behavior of conformal mappings, researcher, Lincoln Labs Hrant Hakobyan, Ph.D.
    [Show full text]
  • Diffusive Estimates for Random Walks on Stationary Random Graphs Of
    Diffusive estimates for random walks on stationary random graphs of polynomial growth Shirshendu Ganguly ∗ James R. Lee y Yuval Peres z Abstract G Let (G; ρ) be a stationary random graph, and use Bρ (r) to denote the ball of radius r about ρ G k in G. Suppose that (G; ρ) has annealed polynomial growth, in the sense that E[ Bρ (r) ] 6 O(r ) for some k > 0 and every r > 1. j j Then there is an infinite sequence of times tn at which the random walk Xt on (G; ρ) is at most diffusive: Almost surely (over the choicef ofg (G; ρ)), there is a number C f> 0g such that h 2 i E distG(X ; Xt ) X = ρ, (G; ρ) 6 Ctn n > 1 : 0 n j 0 8 This result is new even in the case when G is a stationary random subgraph of Zd. Combined with the work of Benjamini, Duminil-Copin, Kozma, and Yadin (2015), it implies that G almost surely does not admit a non-constant harmonic function of sublinear growth. To complement this, we argue that passing to a subsequence of times tn is necessary, as there are stationary random graphs of (almost sure) polynomial growth wheref theg random walk is almost surely superdiffusive at an infinite subset of times. Contents 1 Introduction 2 1.1 The absence of non-constant sublinear growth harmonic functions..........3 1.2 Speed via Euclidean embeddings..............................4 1.3 A deterministic example: Planar graphs..........................6 2 Martingales, embeddings, and growth rates8 2.1 Control by martingales....................................9 2.2 Embeddings and growth rates...............................
    [Show full text]
  • PACKING DIMENSION and CARTESIAN PRODUCTS 1. Introduction Marstrand's Product Theorem
    TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 348, Number 11, November 1996 PACKING DIMENSION AND CARTESIAN PRODUCTS CHRISTOPHER J. BISHOP AND YUVAL PERES Abstract. We show that for any analytic set A in Rd, its packing dimension dimP (A) can be represented as supB dimH (A B) dimH (B) , where the { d × − } supremum is over all compact sets B in R , and dimH denotes Hausdorff dimension. (The lower bound on packing dimension was proved by Tricot in 1982.) Moreover, the supremum above is attained, at least if dimP (A) <d.In contrast, we show that the dual quantity infB dimP (A B) dimP (B) , is at least the “lower packing dimension” of A, but{ can be× strictly− greater.} (The lower packing dimension is greater than or equal to the Hausdorff dimension.) 1. Introduction Marstrand’s product theorem ([9]) asserts that if A, B Rd then ⊂ dim (A B) dim (A)+dim (B), H × ≥ H H where “dimH ” denotes Hausdorff dimension. Refining earlier results of Besicovitch and Moran [3], Tricot [14] showed that (1) dim (A B) dim (B) dim (A) , H × − H ≤ P where “dimP ” denotes packing dimension (see the next section for background). Tricot [15] and also Hu and Taylor [6] asked if this is sharp, i.e., given A,canthe right-hand side of (1) be approximated arbitrarily well by appropriate choices of B on the left-hand side? Our first result, proved in Section 3, states that this is possible. Theorem 1.1. For any analytic set A in Rd (2) sup dimH (A B) dimH (B) =dimP(A), B { × − } where the supremum is over all compact sets B Rd.
    [Show full text]
  • Critical Percolation on Certain Nonunimodular Graphs
    New York Journal of Mathematics New York J. Math. 12 (2006) 1–18. Critical percolation on certain nonunimodular graphs Yuval Peres, G´abor Pete and Ariel Scolnicov Abstract. An important conjecture in percolation theory is that almost sure- ly no infinite cluster exists in critical percolation on any transitive graph for which the critical probability is less than 1. Earlier work has established this for the amenable cases Z2 and Zd for large d, as well as for all nonamenable graphs with unimodular automorphism groups. We show that the conjecture holds for the basic classes of nonamenable graphs with nonunimodular automorphism groups: for decorated trees and the nonunimodular Diestel–Leader graphs. We also show that the connection probability between two vertices decays exponentially in their distance. Finally, we prove that critical percolation on the positive part of the lamplighter group has no infinite clusters. Contents 1. Introduction and preliminaries 1 2. Decorated trees 4 3. Diestel–Leader graphs 8 4. The lamplighter group 14 References 17 1. Introduction and preliminaries 1.1. Introduction. We will focus on the following general conjecture of Benjamini and Schramm [BS96] on critical percolation (see Subsection 1.2 for definitions): Conjecture 1.1. Let G be a transitive graph. If pc < 1, then almost surely critical percolation on G has no infinite clusters. Received February 14, 2005. Mathematics Subject Classification. 60B, 60K, 82B, 20F. Key words and phrases. Critical percolation, nonunimodular, nonamenable, Diestel–Leader graphs, grandmother graph, lamplighter group, decay of connection probability. Our work was partially supported by the NSF grant DMS-0244479 (Peres, Pete), and OTKA (Hungarian National Foundation for Scientific Research) grants T30074 and T049398 (Pete).
    [Show full text]
  • Modern Discrete Probability an Essential Toolkit
    Modern Discrete Probability An Essential Toolkit Sebastien´ Roch November 20, 2014 Modern Discrete Probability: An Essential Toolkit Manuscript version of November 20, 2014 Copyright c 2014 Sebastien´ Roch Contents Preface vi I Introduction 1 1 Models 2 1.1 Preliminaries ............................ 2 1.1.1 Review of graph theory ................... 2 1.1.2 Review of Markov chain theory .............. 2 1.2 Percolation ............................. 2 1.3 Random graphs ........................... 2 1.4 Markov random fields ........................ 2 1.5 Random walks on networks ..................... 3 1.6 Interacting particles on finite graphs ................ 3 1.7 Other random structures ...................... 3 II Basic tools: moments, martingales, couplings 4 2 Moments and tails 5 2.1 First moment method ........................ 6 2.1.1 The probabilistic method .................. 6 2.1.2 Markov’s inequality .................... 8 2.1.3 . Random permutations: longest increasing subsequence . 9 2.1.4 . Constraint satisfaction: bound on random k-SAT threshold 11 2.1.5 . Percolation on Zd: existence of a phase transition .... 12 2.2 Second moment method ...................... 16 2.2.1 Chebyshev’s and Paley-Zygmund inequalities ....... 17 2.2.2 . Erdos-R¨ enyi´ graphs: small subgraph containment .... 21 2.2.3 . Erdos-R¨ enyi´ graphs: connectivity threshold ....... 25 i 2.2.4 . Percolation on trees: branching number, weighted sec- ond moment method, and application to the critical value . 28 2.3 Chernoff-Cramer´ method ...................... 32 2.3.1 Tail bounds via the moment-generating function ..... 33 2.3.2 . Randomized algorithms: Johnson-Lindenstrauss, "-nets, and application to compressed sensing .......... 37 2.3.3 . Information theory: Shannon’s theorem ......... 44 2.3.4 .
    [Show full text]
  • Dimension Theory of Self-Similar Sets and Measures
    Dimension theory of self-similar sets and measures Michael Hochman Abstract We report on recent results about the dimension and smoothness prop- erties of self-similar sets and measures. Closely related to these are results on the linear projections of such sets, and dually, their intersections with ane subspaces. We also discuss recent progress on the the Bernoulli convolutions problem. 1 Introduction Consider a random walk 1 on d, started from a point, and with the (Xn)n=0 R transitions given by Xn+1 = ξnXn, where (ξn) is an independent sequence of similarity maps, chosen according to a xed distribution p. The long term behavior of (Xn) depends on the scaling properties of the ξn. If they are expanding, there is no interesting limit. But the other cases are quite interesting. When the are isometries, and act in some sense irreducibly on d, ξn R both a central limit theorem and local limit theorem hold, i.e. d=2 (Xn −EXn)=n converges in law to a Gaussian, and converges to Lebesgue measure Xn − EXn on bounded open sets [52, 19, 43, 53]. Thus, the limiting behavior is universal, and Xn spreads out as much as possible. The remaining case, namely, when the ξn contract, is our focus here. Then Xn converges in law (without any normalization) to a measure µ, which does not depend on the starting point X0, but very strongly depends on the step distribution p. An important case is when p is nitely supported. The stationary measure µ is called a self-similar measure, and its topological support, which is the set of accumulation points of any orbit of the semigroup generated by supp p, is called a self-similar set.
    [Show full text]