Foliation-Preserving Maps Between Solvmanifolds
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TRANSVERSE STRUCTURE of LIE FOLIATIONS 0. Introduction This
TRANSVERSE STRUCTURE OF LIE FOLIATIONS BLAS HERRERA, MIQUEL LLABRES´ AND A. REVENTOS´ Abstract. We study if two non isomorphic Lie algebras can appear as trans- verse algebras to the same Lie foliation. In particular we prove a quite sur- prising result: every Lie G-flow of codimension 3 on a compact manifold, with basic dimension 1, is transversely modeled on one, two or countable many Lie algebras. We also solve an open question stated in [GR91] about the realiza- tion of the three dimensional Lie algebras as transverse algebras to Lie flows on a compact manifold. 0. Introduction This paper deals with the problem of the realization of a given Lie algebra as transverse algebra to a Lie foliation on a compact manifold. Lie foliations have been studied by several authors (cf. [KAH86], [KAN91], [Fed71], [Mas], [Ton88]). The importance of this study was increased by the fact that they arise naturally in Molino’s classification of Riemannian foliations (cf. [Mol82]). To each Lie foliation are associated two Lie algebras, the Lie algebra G of the Lie group on which the foliation is modeled and the structural Lie algebra H. The latter algebra is the Lie algebra of the Lie foliation F restricted to the clousure of any one of its leaves. In particular, it is a subalgebra of G. We remark that although H is canonically associated to F, G is not. Thus two interesting problems are naturally posed: the realization problem and the change problem. The realization problem is to know which pairs of Lie algebras (G, H), with H subalgebra of G, can arise as transverse and structural Lie algebras, respectively, of a Lie foliation F on a compact manifold M. -
GROUP ACTIONS 1. Introduction the Groups Sn, An, and (For N ≥ 3)
GROUP ACTIONS KEITH CONRAD 1. Introduction The groups Sn, An, and (for n ≥ 3) Dn behave, by their definitions, as permutations on certain sets. The groups Sn and An both permute the set f1; 2; : : : ; ng and Dn can be considered as a group of permutations of a regular n-gon, or even just of its n vertices, since rigid motions of the vertices determine where the rest of the n-gon goes. If we label the vertices of the n-gon in a definite manner by the numbers from 1 to n then we can view Dn as a subgroup of Sn. For instance, the labeling of the square below lets us regard the 90 degree counterclockwise rotation r in D4 as (1234) and the reflection s across the horizontal line bisecting the square as (24). The rest of the elements of D4, as permutations of the vertices, are in the table below the square. 2 3 1 4 1 r r2 r3 s rs r2s r3s (1) (1234) (13)(24) (1432) (24) (12)(34) (13) (14)(23) If we label the vertices in a different way (e.g., swap the labels 1 and 2), we turn the elements of D4 into a different subgroup of S4. More abstractly, if we are given a set X (not necessarily the set of vertices of a square), then the set Sym(X) of all permutations of X is a group under composition, and the subgroup Alt(X) of even permutations of X is a group under composition. If we list the elements of X in a definite order, say as X = fx1; : : : ; xng, then we can think about Sym(X) as Sn and Alt(X) as An, but a listing in a different order leads to different identifications 1 of Sym(X) with Sn and Alt(X) with An. -
Foliations Transverse to Fibers of a Bundle
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 42, Number 2, February 1974 FOLIATIONS TRANSVERSE TO FIBERS OF A BUNDLE J. F. PLANTE Abstract. Consider a fiber bundle where the base space and total space are compact, connected, oriented smooth manifolds and the projection map is smooth. It is shown that if the fiber is null-homologous in the total space, then the existence of a foliation of the total space which is transverse to each fiber and such that each leaf has the same dimension as the base implies that the fundamental group of the base space has exponential growth. Introduction. Let (E, p, B) be a locally trivial fiber bundle where /»:£-*-/? is the projection, E and B are compact, connected, oriented smooth manifolds and p is a smooth map. (By smooth we mean C for some r^l and, henceforth, all maps are assumed smooth.) Let b denote the dimension of B and k denote the dimension of the fiber (thus, dim E= b+k). By a section of the fibration we mean a smooth map a:B-+E such that p o a=idB. It is well known that if a section exists then the fiber over any point in B represents a nontrivial element in Hk(E; Z) since the image of a section is a compact orientable manifold which has intersection number one with the fiber over any point in B. The notion of a section may be generalized as follows. Definition. A polysection of (E,p,B) is a covering projection tr:B-*B together with a map Ç:B-*E such that the following diagram commutes. -
Mathematics of the Rubik's Cube
Mathematics of the Rubik's cube Associate Professor W. D. Joyner Spring Semester, 1996{7 2 \By and large it is uniformly true that in mathematics that there is a time lapse between a mathematical discovery and the moment it becomes useful; and that this lapse can be anything from 30 to 100 years, in some cases even more; and that the whole system seems to function without any direction, without any reference to usefulness, and without any desire to do things which are useful." John von Neumann COLLECTED WORKS, VI, p. 489 For more mathematical quotes, see the first page of each chapter below, [M], [S] or the www page at http://math.furman.edu/~mwoodard/mquot. html 3 \There are some things which cannot be learned quickly, and time, which is all we have, must be paid heavily for their acquiring. They are the very simplest things, and because it takes a man's life to know them the little new that each man gets from life is very costly and the only heritage he has to leave." Ernest Hemingway (From A. E. Hotchner, PAPA HEMMINGWAY, Random House, NY, 1966) 4 Contents 0 Introduction 13 1 Logic and sets 15 1.1 Logic................................ 15 1.1.1 Expressing an everyday sentence symbolically..... 18 1.2 Sets................................ 19 2 Functions, matrices, relations and counting 23 2.1 Functions............................. 23 2.2 Functions on vectors....................... 28 2.2.1 History........................... 28 2.2.2 3 × 3 matrices....................... 29 2.2.3 Matrix multiplication, inverses.............. 30 2.2.4 Muliplication and inverses............... -
FOLIATIONS Introduction. the Study of Foliations on Manifolds Has a Long
BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 80, Number 3, May 1974 FOLIATIONS BY H. BLAINE LAWSON, JR.1 TABLE OF CONTENTS 1. Definitions and general examples. 2. Foliations of dimension-one. 3. Higher dimensional foliations; integrability criteria. 4. Foliations of codimension-one; existence theorems. 5. Notions of equivalence; foliated cobordism groups. 6. The general theory; classifying spaces and characteristic classes for foliations. 7. Results on open manifolds; the classification theory of Gromov-Haefliger-Phillips. 8. Results on closed manifolds; questions of compact leaves and stability. Introduction. The study of foliations on manifolds has a long history in mathematics, even though it did not emerge as a distinct field until the appearance in the 1940's of the work of Ehresmann and Reeb. Since that time, the subject has enjoyed a rapid development, and, at the moment, it is the focus of a great deal of research activity. The purpose of this article is to provide an introduction to the subject and present a picture of the field as it is currently evolving. The treatment will by no means be exhaustive. My original objective was merely to summarize some recent developments in the specialized study of codimension-one foliations on compact manifolds. However, somewhere in the writing I succumbed to the temptation to continue on to interesting, related topics. The end product is essentially a general survey of new results in the field with, of course, the customary bias for areas of personal interest to the author. Since such articles are not written for the specialist, I have spent some time in introducing and motivating the subject. -
Lecture Notes on Foliation Theory
INDIAN INSTITUTE OF TECHNOLOGY BOMBAY Department of Mathematics Seminar Lectures on Foliation Theory 1 : FALL 2008 Lecture 1 Basic requirements for this Seminar Series: Familiarity with the notion of differential manifold, submersion, vector bundles. 1 Some Examples Let us begin with some examples: m d m−d (1) Write R = R × R . As we know this is one of the several cartesian product m decomposition of R . Via the second projection, this can also be thought of as a ‘trivial m−d vector bundle’ of rank d over R . This also gives the trivial example of a codim. d- n d foliation of R , as a decomposition into d-dimensional leaves R × {y} as y varies over m−d R . (2) A little more generally, we may consider any two manifolds M, N and a submersion f : M → N. Here M can be written as a disjoint union of fibres of f each one is a submanifold of dimension equal to dim M − dim N = d. We say f is a submersion of M of codimension d. The manifold structure for the fibres comes from an atlas for M via the surjective form of implicit function theorem since dfp : TpM → Tf(p)N is surjective at every point of M. We would like to consider this description also as a codim d foliation. However, this is also too simple minded one and hence we would call them simple foliations. If the fibres of the submersion are connected as well, then we call it strictly simple. (3) Kronecker Foliation of a Torus Let us now consider something non trivial. -
Commentary on Thurston's Work on Foliations
COMMENTARY ON FOLIATIONS* Quoting Thurston's definition of foliation [F11]. \Given a large supply of some sort of fabric, what kinds of manifolds can be made from it, in a way that the patterns match up along the seams? This is a very general question, which has been studied by diverse means in differential topology and differential geometry. ... A foliation is a manifold made out of striped fabric - with infintely thin stripes, having no space between them. The complete stripes, or leaves, of the foliation are submanifolds; if the leaves have codimension k, the foliation is called a codimension k foliation. In order that a manifold admit a codimension- k foliation, it must have a plane field of dimension (n − k)." Such a foliation is called an (n − k)-dimensional foliation. The first definitive result in the subject, the so called Frobenius integrability theorem [Fr], concerns a necessary and sufficient condition for a plane field to be the tangent field of a foliation. See [Spi] Chapter 6 for a modern treatment. As Frobenius himself notes [Sa], a first proof was given by Deahna [De]. While this work was published in 1840, it took another hundred years before a geometric/topological theory of foliations was introduced. This was pioneered by Ehresmann and Reeb in a series of Comptes Rendus papers starting with [ER] that was quickly followed by Reeb's foundational 1948 thesis [Re1]. See Haefliger [Ha4] for a detailed account of developments in this period. Reeb [Re1] himself notes that the 1-dimensional theory had already undergone considerable development through the work of Poincare [P], Bendixson [Be], Kaplan [Ka] and others. -
An Algebraic Approach to the Weyl Groupoid
An Algebraic Approach to the Weyl Groupoid Tristan Bice✩ Institute of Mathematics Czech Academy of Sciences Zitn´a25,ˇ 115 67 Prague, Czech Republic Abstract We unify the Kumjian-Renault Weyl groupoid construction with the Lawson- Lenz version of Exel’s tight groupoid construction. We do this by utilising only a weak algebraic fragment of the C*-algebra structure, namely its *-semigroup reduct. Fundamental properties like local compactness are also shown to remain valid in general classes of *-rings. Keywords: Weyl groupoid, tight groupoid, C*-algebra, inverse semigroup, *-semigroup, *-ring 2010 MSC: 06F05, 20M25, 20M30, 22A22, 46L05, 46L85, 47D03 1. Introduction 1.1. Background Renault’s groundbreaking thesis [Ren80] revealed the striking interplay be- tween ´etale groupoids and the C*-algebras they give rise to. Roughly speaking, the ´etale groupoid provides a more topological picture of the corresponding C*-algebra, with various key properties of the algebra, like nuclearity and sim- plicity (see [ADR00] and [CEP+19]), being determined in a straightforward way from the underlying ´etale groupoid. Naturally, this has led to the quest to find appropriate ´etale groupoid models for various C*-algebras. Two general methods have emerged for finding such models, namely arXiv:1911.08812v3 [math.OA] 20 Sep 2020 1. Exel’s tight groupoid construction from an inverse semigroup, and 2. Kumjian-Renault’s Weyl groupoid construction from a Cartan C*-subalgebra (see [Exe08], [Kum86] and [Ren08]). However, both of these have their limi- tations. For example, tight groupoids are always ample, which means the cor- responding C*-algebras always have lots of projections. On the other hand, the Weyl groupoid is always effective, which discounts many naturally arising groupoids. -
A Class of Totally Geodesic Foliations of Lie Groups
Proc. Indian Acad. Sci. (Math. Sci.), Vol. 100, No. 1, April 1990, pp. 57-64. ~2 Printed in India. A class of totally geodesic foliations of Lie groups G SANTHANAM School of Mathematics. Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India MS received 4 October 1988; revised 25 May 1989 A~traet. This paper is devoted to classifying the foliations of G with leaves of the form .qKh - t where G is a compact, connected and simply connected L,c group and K is a connected closed subgroup of G such that G/K is a rank-I Riemannian symmetric space. In the case when G/K =S", the homotopy type of space of such foliations is also given. Keywords. Foliations; rank-I Riemannian symmetric space; cutlocus. I. Introduction The study of fibrations of spheres by great spheres is a very interesting problem in geometry and it is very important in the theory of Blaschke manifolds. In [l], Gluck and Warner have studied the great circle fibrations of the three spheres. In that paper they have proved very interesting results. When we look at the problem group theoretically, we see that all the results of [1] go through, for foliations of G with leaves of the form gKh- 1 where G is a compact, connected and simply connected Lie group and K is a connected closed subgroup of G such that G/K is a rank- l Riemannian symmetric space (see [-2]), except perhaps the theorem 3 for the pair (G, K) such that G/K=CP n, HP ~ etc. -
Hyperbolic Metrics, Measured Foliations and Pants Decompositions for Non-Orientable Surfaces Athanase Papadopoulos, Robert C
Hyperbolic metrics, measured foliations and pants decompositions for non-orientable surfaces Athanase Papadopoulos, Robert C. Penner To cite this version: Athanase Papadopoulos, Robert C. Penner. Hyperbolic metrics, measured foliations and pants de- compositions for non-orientable surfaces. Asian Journal of Mathematics, International Press, 2016, 20 (1), p. 157-182. 10.4310/AJM.2016.v20.n1.a7. hal-00856638v3 HAL Id: hal-00856638 https://hal.archives-ouvertes.fr/hal-00856638v3 Submitted on 1 Oct 2013 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. HYPERBOLIC METRICS, MEASURED FOLIATIONS AND PANTS DECOMPOSITIONS FOR NON-ORIENTABLE SURFACES A. PAPADOPOULOS AND R. C. PENNER Abstract. We provide analogues for non-orientable surfaces with or without boundary or punctures of several basic theorems in the setting of the Thurston theory of surfaces which were developed so far only in the case of orientable surfaces. Namely, we pro- vide natural analogues for non-orientable surfaces of the Fenchel- Nielsen theorem on the parametrization of the Teichm¨uller space of the surface, the Dehn-Thurston theorem on the parametrization of measured foliations in the surface, and the Hatcher-Thurston theorem, which gives a complete minimal set of moves between pair of pants decompositions of the surface. -
Distortion of Dimension by Metric Space-Valued Sobolev Mappings Lecture II
Distortion of dimension by metric space-valued Sobolev mappings Lecture II Jeremy Tyson University of Illinois at Urbana-Champaign Metric Spaces: Analysis, Embeddings into Banach Spaces, Applications Texas A&M University College Station, TX 8 July 2016 Outline Lecture I. Sobolev and quasiconformal mappings in Euclidean space Lecture II. Sobolev mappings between metric spaces Lecture III. Dimension distortion theorems for Sobolev and quasiconformal mappings defined from the sub-Riemannian Heisenberg group f homeo in Rn, n ≥ 2 Gehring metric QC ) analytic QC ) geometric QC modulus) estimates (local) QS f : X ! Y homeo between proper Q-regular mms satisfying Q-PI, Q > 1 0 metric QC HK=)98 QS f : X ! Y homeo between proper Q-regular mms 0 . geometric QC T(98 QS Motivation: quasiconformal mappings in metric spaces The theory of analysis in metric measure spaces originates in two papers of Juha Heinonen and Pekka Koskela: ‘Definitions of quasiconformality', Invent. Math., 1995 `QC maps in metric spaces of controlled geometry', Acta Math., 1998 The latter paper introduced the concept of p-Poincar´einequality on a metric measure space, which has become the standard axiom for first-order analysis. f : X ! Y homeo between proper Q-regular mms satisfying Q-PI, Q > 1 0 metric QC HK=)98 QS f : X ! Y homeo between proper Q-regular mms 0 . geometric QC T(98 QS Motivation: quasiconformal mappings in metric spaces The theory of analysis in metric measure spaces originates in two papers of Juha Heinonen and Pekka Koskela: ‘Definitions of quasiconformality', Invent. Math., 1995 `QC maps in metric spaces of controlled geometry', Acta Math., 1998 The latter paper introduced the concept of p-Poincar´einequality on a metric measure space, which has become the standard axiom for first-order analysis. -
Sculpting with Fiber Bundle and Foliation
Sculpting with Fiber Bundle and Foliation Hang Li, Zhipei Yan May, 2016 1 Theory Definition 1.1. For space E(total space), B(base), F (fiber) and surjection π : E ! B (1) if there is an open neighborhood U of π(x) (x 2 E) such that π−1(U) and U × F are homeomorphic, (E; B; F; π) is a fiber bundle. And E has the form of product space B × F . Figure 1: Base and Fiber Here are two kinds of fiber bundle on a torus. Figure 2: Trivial Fibers Figure 3: Nontrivial Fibers 1 Definition 1.2. fUig is an atlas of an n-dimensional manifold U. For each chart Ui, define n φi : Ui ! R (2) If Ui \ Uj 6= ;, define −1 'ij = φj ◦ φi (3) And if 'ij has the form of 1 2 'ij = ('ij(x);'ij(x; y)) (4) 1 n−p n−p 'ij : R ! R (5) 2 n p 'ij : R ! R (6) then for any stripe si : x = ci in Ui there must be a stripe in Uj sj : x = cj such that si and sj are the same curve in Ui \ Uj and can be connected. The maximal connection is a leaf. This structure is called a p-dimensional foliation F of an n-dimensional manifold U. Property 1.1. All the fiber bundles compose a group GF = (fFig; ◦). If we regard the fiber bundle(1-manifold) as a parameterization on a surface(2-manifold), we can prove it easily. As an example, we use the parameterization on a torus.