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MEMOIRS of the American Mathematical Society Volume 241 • Number 1141 (second of 4 numbers) • May 2016 Group Colorings and Bernoulli Subflows Su Gao Steve Jackson Brandon Seward ISSN 0065-9266 (print) ISSN 1947-6221 (online) American Mathematical Society MEMOIRS of the American Mathematical Society Volume 241 • Number 1141 (second of 4 numbers) • May 2016 Group Colorings and Bernoulli Subflows Su Gao Steve Jackson Brandon Seward ISSN 0065-9266 (print) ISSN 1947-6221 (online) American Mathematical Society Providence, Rhode Island Library of Congress Cataloging-in-Publication Data Names: Gao,Su,1968–—Jackson,Steve,1957–—Seward,Brandon,1987– Title: GroupcoloringsandBernoullisubflows/SuGao,SteveJackson,BrandonSeward. Description: Providence,RhodeIsland: AmericanMathematicalSociety,2016. —Series: Mem- oirsoftheAmericanMathematicalSociety,ISSN0065-9266;volume241,number1141—Includes bibliographicalreferencesandindex. Identifiers: LCCN2015051377—ISBN9781470418472(alk. paper) Subjects: LCSH:Fluidmechanics. —Bernoullinumbers. Classification: LCC QA901.G372016—DDC512.7–dc23LC recordavailable athttp://lccn. loc.gov/2015051377 DOI:http://dx.doi.org/10.1090/memo/1141 Memoirs of the American Mathematical Society Thisjournalisdevotedentirelytoresearchinpureandappliedmathematics. Subscription information. Beginning with the January 2010 issue, Memoirs is accessible from www.ams.org/journals. The 2016 subscription begins with volume 239 and consists of six mailings, each containing one or more numbers. Subscription prices for 2016 are as follows: for paperdelivery,US$890list,US$712.00institutionalmember;forelectronicdelivery,US$784list, US$627.20institutional member. Uponrequest, subscribers topaper delivery ofthis journalare also entitled to receive electronic delivery. If ordering the paper version, add US$10 for delivery withintheUnitedStates;US$69foroutsidetheUnitedStates. Subscriptionrenewalsaresubject tolatefees. Seewww.ams.org/help-faqformorejournalsubscriptioninformation. Eachnumber maybeorderedseparately;please specifynumber whenorderinganindividualnumber. Back number information. Forbackissuesseewww.ams.org/backvols. Subscriptions and orders should be addressed to the American Mathematical Society, P.O. Box 845904, Boston, MA 02284-5904USA. All orders must be accompanied by payment. Other correspondenceshouldbeaddressedto201CharlesStreet,Providence,RI02904-2294USA. Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy select pages for useinteachingorresearch. Permissionisgrantedtoquotebriefpassagesfromthispublicationin reviews,providedthecustomaryacknowledgmentofthesourceisgiven. Republication,systematiccopying,ormultiplereproductionofanymaterialinthispublication is permitted only under license from the American Mathematical Society. Permissions to reuse portions of AMS publication content are handled by Copyright Clearance Center’s RightsLink(cid:2) service. Formoreinformation,pleasevisit: http://www.ams.org/rightslink. Sendrequestsfortranslationrightsandlicensedreprintstoreprint-permission@ams.org. Excludedfromtheseprovisionsismaterialforwhichtheauthorholdscopyright. Insuchcases, requestsforpermissiontoreuseorreprintmaterialshouldbeaddresseddirectlytotheauthor(s). Copyrightownershipisindicatedonthecopyrightpage,oronthelowerright-handcornerofthe firstpageofeacharticlewithinproceedingsvolumes. MemoirsoftheAmericanMathematicalSociety (ISSN0065-9266(print);1947-6221(online)) ispublishedbimonthly(eachvolumeconsistingusuallyofmorethanonenumber)bytheAmerican MathematicalSocietyat201CharlesStreet,Providence,RI02904-2294USA.Periodicalspostage paid at Providence, RI.Postmaster: Send address changes to Memoirs, AmericanMathematical Society,201CharlesStreet,Providence,RI02904-2294USA. (cid:2)c 2015bytheAmericanMathematicalSociety. Allrightsreserved. (cid:2) ThispublicationisindexedinMathematicalReviewsR,Zentralblatt MATH,ScienceCitation Index(cid:2)R,ScienceCitation IndexTM-Expanded,ISI Alerting ServicesSM,SciSearch(cid:2)R,Research (cid:2) (cid:2) (cid:2) AlertR,CompuMathCitation IndexR,Current ContentsR/Physical, Chemical& Earth Sciences. ThispublicationisarchivedinPortico andCLOCKSS. PrintedintheUnitedStatesofAmerica. (cid:2)∞ Thepaperusedinthisbookisacid-freeandfallswithintheguidelines establishedtoensurepermanenceanddurability. VisittheAMShomepageathttp://www.ams.org/ 10987654321 201918171615 Contents Chapter 1. Introduction 1 1.1. Bernoulli flows and subflows 1 1.2. Basic notions 3 1.3. Existence of free subflows 4 1.4. Hyper aperiodic points and k-colorings 6 1.5. Complexity of sets and equivalence relations 9 1.6. Tilings of groups 11 1.7. The almost equality relation 12 1.8. The fundamental method 14 1.9. Brief outline 16 Chapter 2. Preliminaries 19 2.1. Bernoulli flows 19 2.2. 2-colorings 21 2.3. Orthogonality 23 2.4. Minimality 24 2.5. Strengthening and weakening of 2-colorings 27 2.6. Other variations of 2-colorings 30 2.7. Subflows of (2N)G 32 Chapter 3. Basic Constructions of 2-Colorings 35 3.1. 2-Colorings on supergroups of finite index 35 3.2. 2-Colorings on group extensions 39 3.3. 2-Colorings on Z 43 3.4. 2-Colorings on nonabelian free groups 46 3.5. 2-Colorings on solvable groups 48 3.6. 2-Colorings on residually finite groups 51 Chapter 4. Marker Structures and Tilings 53 4.1. Marker structures on groups 53 4.2. 2-Colorings on abelian and FC groups by markers 57 4.3. Some properties of ccc groups 61 4.4. Abelian, nilpotent, and polycyclic groups are ccc 63 4.5. Residually finite and locally finite groups and free products are ccc 70 Chapter 5. Blueprints and Fundamental Functions 77 5.1. Blueprints 77 5.2. Fundamental functions 84 5.3. Existence of blueprints 91 5.4. Growth of blueprints 98 iii iv CONTENTS Chapter 6. Basic Applications of the Fundamental Method 103 6.1. The uniform 2-coloring property 103 6.2. Density of 2-colorings 107 6.3. Characterization of the ACP 109 Chapter 7. Further Study of Fundamental Functions 117 7.1. Subflows generated by fundamental functions 117 7.2. Pre-minimality 122 7.3. Δ-minimality 127 7.4. Minimality constructions 131 7.5. Rigidity constructions for topological conjugacy 138 Chapter 8. The Descriptive Complexity of Sets of 2-Colorings 147 8.1. Smallness in measure and category 147 8.2. Σ0-hardness and Π0-completeness 148 2 3 8.3. Flecc groups 151 8.4. Nonflecc groups 156 Chapter 9. The Complexity of the Topological Conjugacy Relation 169 9.1. Introduction to countable Borel equivalence relations 169 9.2. Basic properties of topological conjugacy 170 9.3. Topological conjugacy of minimal free subflows 176 9.4. Topological conjugacy of free subflows 185 Chapter 10. Extending Partial Functions to 2-Colorings 205 10.1. A sufficient condition for extendability 205 10.2. A characterization for extendability 207 10.3. Almost equality and cofinite domains 218 10.4. Automatic extendability 229 Chapter 11. Further Questions 233 11.1. Group structures 233 11.2. 2-colorings 234 11.3. Generalizations 235 11.4. Descriptive complexity 236 Bibliography 237 Index 239 Abstract InthispaperwestudythedynamicsofBernoulliflowsandtheirsubflows over general countable groups. One of the main themes of this paper is to establish the correspondence between the topological and the symbolic perspectives. From the topological perspective, we are particularly interested in free subflows (subflows in whicheverypointhastrivialstabilizer), minimal subflows, disjointness ofsubflows, andtheproblemofclassifyingsubflows uptotopologicalconjugacy. Ourmaintool to study free subflows will be the notion of hyper aperiodic points; a point is hyper aperiodic if the closure of its orbit is a free subflow. We show that the notion of hyper aperiodicity corresponds to a notion of k-coloring on the countable group, a key notion we study throughout the paper. In fact, for all important topological notionswestudy,correspondingnotionsingroupcombinatoricswillbeestablished. Conversely, many variations of the notions in group combinatorics are proved to be equivalent to some topological notions. In particular, we obtain results about the differences in dynamical properties between pairs of points which disagree on finitely many coordinates. Another main theme of the paper is to study the properties of free subflows and minimal subflows. Again this is done through studying the properties of the hyper aperiodic points and minimal points. We prove that the set of all (minimal) hyper aperiodic points is always dense but meager and null. By employing notions and ideas from descriptive set theory, we study the complexity of the sets of hyper aperiodicpoints and of minimal points, and completely determine their descriptive ReceivedbytheeditorDecember28,2011and,inrevisedform,May19,2014. ArticleelectronicallypublishedonDecember10,2015. DOI:http://dx.doi.org/10.1090/memo/1141 2010 Mathematics Subject Classification. Primary37B10,20F99;Secondary 03E15,37B05, 20F65. Key words and phrases. Colorings, hyper aperiodic points, orthogonal colorings, Bernoulli flows, Bernoulli shifts, Bernoulli subflows, free subflows, marker structures, tilings, topological conjugacy. SuGao’sresearchwassupportedbytheU.S.NSFGrantsDMS-0501039andDMS-0901853. SteveJackson’sresearchwassupportedbytheU.S.NSFGrantDMS-0901853. BrandonSeward’sresearchwassupportedbytwoREUsupplementstotheU.S.NSFGrant DMS-0501039andanNSFGraduateResearchFellowship. Su Gao is affiliated with the Department of Mathematics, University of North Texas, 1155 UnionCircle#311430,Denton,Texas76203-5017. E-mail: [email protected]. SteveJacksonisaffiliatedwiththeDepartmentofMathematics,UniversityofNorthTexas, 1155UnionCircle#311430,Denton,Texas76203-5017. E-mail: [email protected]. Brandon Seward is affiliated with theDepartment of Mathematics, University of Michigan, 530ChurchStreet,AnnArbor,Michigan48109-1043. E-mail: [email protected]. (cid:2)c2015 American Mathematical Society v vi ABSTRACT complexity. In doing this we introduce a new notion of countable flecc groups and study their properties. We also obtain the following results for the classification problem of free subflows up to topological conjugacy. For locally finite groups the topological conjugacy relation for all (free) subflows is hyperfinite and nonsmooth. For nonlocally finite groups the relation is Borel bireducible with the universal countable Borel equivalence relation. The third, but not the least important, theme of the paper is to develop con- structive methods for the notions studied. To construct k-colorings on countable groups, a fundamental method of construction of multi-layer marker structures is developed with great generality. This allows one to construct an abundance of k- colorings with specific properties. Variations of the fundamental method are used in many proofs in the paper, and we expect them to be useful more broadly in geometric group theory. As a special case of such marker structures, we study the notion of ccc groups and prove the ccc-ness for countable nilpotent, polycyclic, residually finite, locally finite groups and for free products. CHAPTER 1 Introduction In this paper we study Bernoulli flows over arbitrary countable groups (these are also known as Bernoulli shifts, Bernoulli systems, and Bernoulli schemes). The overall focus of this paper is on the development and application of constructive methods, with a particular emphasis on questions surrounding free subflows. The topics, methods, and results presented here should be of interest to at least re- searchers in descriptive set theory, symbolic dynamics, and topological dynamics, and may be of interest to researchers in C∗-algebras, ergodic theory, geometric group theory, and percolation theory. In Section 1.1 we remind the reader the def- initions of Bernoulli flow and subflow and also discuss the importance of Bernoulli flowstovariousareasofmathematics. InSection1.2weintroducesomebasicnota- tionandterminologywhichisneededforthischapter. InSection1.3wediscussthe questionoftheexistenceoffreesubflows. Thisquestionhasbeenrecentlyanswered and is of importance to this paper. In Sections 1.4, 1.5, 1.6, and 1.7 we discuss the main results of this paper and at the same time discuss relevance to and mo- tivation from various areas of mathematics, namely descriptive set theory, ergodic theory, geometric group theory, symbolic dynamics, and topological dynamics. A significant aspect of this paper is the invention of some versatile tools which add structure to arbitrary countable groups and offer significant aid in constructing points in Bernoulli flows. These tools are developed in great generality and likely have applications beyondtheir use here. These constructivemethods and their po- tential utility tovarious areas of mathematics are discussed inSection 1.8. Finally, inSection1.9wegiveabriefoutlinetothepaperanddiscusschapterdependencies. We encourage the reader to make use of the detailed index found at the end of the paper which includes both terminology and notation. 1.1. Bernoulli flows and subflows Let us first begin by presenting the most general definition of a Bernoulli flow (also known as Bernoulli shift, Bernoulli system, and Bernoulli scheme). If G is a countable group and K is a set with the discrete topology and with a probability measure ν, then the Bernoulli flow over G with alphabet K is defined to be (cid:2) KG ={x : G→K}= K g∈G together with the product topology, the product measure νG, and the following action of G: for x∈KG and g ∈G, g·x∈KG is defined by (g·x)(h)=x(g−1h). ThesetK isalwaysassumedtohaveatleasttwoelementsasotherwiseKG consists of a single point. TheactionofGonKG isquiteintuitive. Forexample,ifG=ZandK ={0,1} thenKG ={0,1}Z canbe viewedasthespace of all bi-infinite sequencesof0’s and 1 2 1. INTRODUCTION 1’s. Z then acts by shifting these sequences left and right (the action of 5 ∈ Z shifts these sequences 5 units to the right). Similarly, {0,1}Z2 can be visualized as thespace of{0,1}-labelings of the twodimensional latticeZ2 ⊆R2 withtheaction of Z2 moving the labels in the obvious fashion. Comprehension of these examples should lead to an intuitive understanding of the action of G on KG. Under theproducttopology, thebasic opensetsofKG arethe setsof theform {x∈KG : ∀1≤i≤n x(h )=k } i i where h ,h ,...,h ∈ G, k ,k ,...,k ∈ K, and n ≥ 1. Thus the action of G on 1 2 n 1 2 n KG is continuous. It is not difficult to see that the basic open sets of KG are both open and closed (i.e. clopen). Since every point is the intersection of a decreasing sequence of basic open sets, it follows that KG is totally disconnected (meaning that the only connected sets are the one point sets). KG is also seen to be perfect (meaning that there are no isolated points). Furthermore, KG is compact if and onlyifK isfinite. Thusbyawellknowntheoremoftopology,KG ishomeomorphic tothe Cantor set wheneverK is finite. Onbasic opensets the measure νG is given by (cid:2) νG({x∈KG : ∀1≤i≤n x(h )=k })= ν(k ). i i i 1≤i≤n Therefore the action of G on KG is measure preserving. It may not be so clear, but this action is in fact ergodic. InadditiontoBernoulliflows,wearealsoveryinterestedintheirsubflows (also known as subshifts or subsystems). A subflow of a Bernoulli flow KG is simply a closed subset of KG which is stable under the action of G. Bernoulli flows and their subflows show up in many areas of mathematics. One reason is that they have a rich diversity of dynamical properties which allow them to model many phenomenon. This “modeling” shows up in many contexts, such as in ergodic theory, descriptive set theory, percolation theory, topological dynamics, and sym- bolic dynamics. In ergodic theory and descriptive set theory, the orbit structures of Bernoulli flows are used to model the orbit structures of measurable group ac- tions on other measure spaces. More generally, they are used to model countable Borel equivalence relations as a well known result of Feldman-Moore states that every countable Borel equivalence relation on a standard Borel space is induced by a Borel action of a countable group ([FM]). In the site percolation model of percolation theory, Bernoulli flows of the form {0,1}G are used to model the flow of liquids through porous materials. In topological dynamics, it is known that if a group G acts continuously on a compact topological space X and the action is expansive, then there is a Bernoulli flow KG over G, a subflow S ⊆ KG, and a continuous surjection φ : S → X which commutes with the action of G (meaning φ(g·s)=g·φ(s)forallg ∈Gands∈S). Furthermore,ifX istotallydisconnected then φ can be chosen to be a homeomorphism. Similarly, if X can be partitioned by a collection of clopen sets, then there is a subflow S of a Bernoulli flow KG and a continuous surjection φ : X → S which commutes with the action of G. These typesoffactscanbeusedtostudyBernoulliflowsviatopologicaldynamics(forex- ample, asin[GU]),butmorefrequentlytopologicaldynamicalsystemsarestudied viaBernoulliflows. Thislatterapproach ledtotheinvention ofsymbolic dynamics ([MH])anditssubsequentgrowthoverthepastseventyyears. Aclassicalexample of the use of symbolic dynamics is the modeling of geodesics flows on manifolds by 1.2. BASIC NOTIONS 3 (thesuspension of)subflows of Bernoulli flows overZ. Traditionally only Bernoulli flows over Z and Zn are studied insymbolic dynamics, but more recently Bernoulli flows over hyperbolic groups have been used to model the dynamics of hyperbolic groups acting on their boundary ([CP]). AkeyaspectoftheimportanceofBernoulliflowsistheirmodelingcapabilities, but there are several other reasons to study them as well. Indeed, Bernoulli flows may be considered interesting in and of themselves. This viewpoint can be seen in at least descriptive set theory, ergodic theory, and symbolic dynamics. Bernoulli flows serve as very natural examples of orbit equivalence relations, of measure pre- serving ergodic group actions, and of continuous group actions on compact spaces. At the same time, Bernoulli flows have very simple definitions yet their dynamical propertiesareverydifficulttofullyunderstand. Aparticularlyniceandmanytimes useful aspect of Bernoulli flows is that they are susceptible to combinatorial argu- ments, something which is typically not seen in other dynamical systems. Indeed, combinatorial approaches are a predominant feature both in symbolic dynamics and in this paper. Another source of motivation for studying Bernoulli flows is to understand the relationship between the algebraic properties of the acting group and the dynamical properties of the Bernoulli flow (a research program suggested by Gottschalk in [Go]). There are some known results of this type. For example, with complete knowledge of the dynamical properties of a Bernoulli flow KG, one candetermineifGisamenable([CFW]),ifGhasKazhdan’sproperty(T)([GW]), and the rank of G if G is a nonabelian free group ([Ga]), to name a few. This is another aspect of Bernoulli flows which appears on several occasions in this paper. Finally, in topological dynamics Bernoulli flows are also studied in order to reveal properties of the greatest ambit of G, since it is known that the greatest ambit of G is the enveloping semigroup of the Bernoulli flow {0,1}G (see [GU]). In this paper we study the dynamics of Bernoulli flows from the symbolic and topologicalviewpointsandemployideasfromdescriptivesettheorytogainfurther understanding. Although we do not study Bernoulli flows from the ergodic theory perspective, there is a topic we study (tileability properties of groups) which could be of interest to researchers in ergodic theory and geometric group theory. 1.2. Basic notions We study Bernoulli flows from the symbolic and topological perspectives. We therefore only want to consider Bernoulli flows over finite alphabets (these are precisely the compact Bernoulli flows, as mentioned in the previous section). So throughout the paper the term “Bernoulli flow” will always mean “Bernoulli flow over a finite alphabet.” We will also not make use of any measures (aside from a single lemma). So we will never specify measures on the alphabets or on the Bernoulli flows. Since the alphabet K is always finite and the particular elements of K are unimportant, we will always use K = {0,1,...,k−1} for some positive integer k >1. As is common in logic and descriptive set theory, we let the positive integerkdenotetheset{0,1,...,k−1}. WethereforewritekG ={0,1,...,k−1}G. Let G be a countable group and let X be a compact Hausdorff space on which G acts continuously (such as the Bernoulli flow kG). A closed subset of X which is stable under the group action is called a subflow of X. We denote the closure of sets A⊆X by A. If x∈X, then the orbit of x is denoted [x]={g·x : g ∈G}.

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