DOCSLIB.ORG

Distortion of Dimension by Sobolev and Quasiconformal Mappings

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Distortion of Dimension by Sobolev and Quasiconformal Mappings Distortion of dimension by Sobolev and quasiconformal mappings J. Tyson 18 June 2014 I. Introduction and overview, quasiconformal maps of Rn and their effect on Hausdorff dimension II. Global quasiconformal dimension in Rn III. Conformal dimension of metric spaces IV. Sobolev dimension distortion in Rn and in metric spaces V. QC and Sobolev dimension distortion in the sub-Riemannian Heisenberg group 1 In this final lecture we will survey known results on distortion of dimension by Sobolev and quasiconformal mappings of the sub-Riemannian Heisenberg group Hn. n We equip H with the Carnot-Carath´eodory metric dcc and recall that the n Hausdorff dimension of (H ; dcc ) is Q = 2n + 2. A homeomorphism f :Ω ! Ω0 between domains in Hn is (metrically) K-quasiconformal if supfdcc (f (p); f (q)) : dcc (p; q) = rg lim sup 0 0 ≤ K 8 p 2 Ω: r!0 inffdcc (f (p); f (q )) : dcc (p; q ) = rg 2 A major difficulty, however, lies in the lack of effective methods for constructing Heisenberg quasiconformal maps. For instance, • naive versions of the radial stretch map x 7! jxja−1x fail to be quasiconformal (cf. recent work of Balogh{F¨assler{Platis), • PL techniques are not obviously available, • no theory of Heisenberg quasiuniform convexity exists to date. Many results of the Euclidean theory of quasiconformal maps carry over to the Heisenberg group (and even to more general metric measure spaces). 3 Many results of the Euclidean theory of quasiconformal maps carry over to the Heisenberg group (and even to more general metric measure spaces). A major difficulty, however, lies in the lack of effective methods for constructing Heisenberg quasiconformal maps. For instance, • naive versions of the radial stretch map x 7! jxja−1x fail to be quasiconformal (cf. recent work of Balogh{F¨assler{Platis), • PL techniques are not obviously available, • no theory of Heisenberg quasiuniform convexity exists to date. 4 1. For each 0 < s < t < Q there exists E ⊂ Hn compact and f : Hn ! Hn qc s.t. dim E = s and dim f (E) = t. f 2. Gehring{V¨ais¨al¨atheorem: for each 0 < s < Q and K ≥ 1 9 0 < β ≤ α < Q s.t. β ≤ dim f (E) ≤ α whenever E ⊂ Hn with dim E = s and f is K-qc. Distortion of dimension by quasiconformal maps in Hn Z. M. Balogh, \Hausdorff dimension distribution of quasiconformal mappings on the Heisenberg group", J. d'Analyse Math. (2001) 5 f 2. Gehring{V¨ais¨al¨atheorem: for each 0 < s < Q and K ≥ 1 9 0 < β ≤ α < Q s.t. β ≤ dim f (E) ≤ α whenever E ⊂ Hn with dim E = s and f is K-qc. Distortion of dimension by quasiconformal maps in Hn Z. M. Balogh, \Hausdorff dimension distribution of quasiconformal mappings on the Heisenberg group", J. d'Analyse Math. (2001) 1. For each 0 < s < t < Q there exists E ⊂ Hn compact and f : Hn ! Hn qc s.t. dim E = s and dim f (E) = t. 6 f Distortion of dimension by quasiconformal maps in Hn Z. M. Balogh, \Hausdorff dimension distribution of quasiconformal mappings on the Heisenberg group", J. d'Analyse Math. (2001) 1. For each 0 < s < t < Q there exists E ⊂ Hn compact and f : Hn ! Hn qc s.t. dim E = s and dim f (E) = t. 2. Gehring{V¨ais¨al¨atheorem: for each 0 < s < Q and K ≥ 1 9 0 < β ≤ α < Q s.t. β ≤ dim f (E) ≤ α whenever E ⊂ Hn with dim E = s and f is K-qc. 7 Proof sketch: For s ≤ 2n + 1, choose E to be the union of line segments along integral curves of the horiz vector field X1 emanating from a Cantor set in the z2 ··· znt-subspace. Criteria of the Bourdon{Pansu theorem hold. S For 2n + 1 ≤ s ≤ Q, let E = r2C @BH (o; r) be a Cantor set's worth of Kor´anyi n spheres @BH (o; r) = fp 2 H : dH (o; p) = rg. Apply a version of the Bourdon{Pansu criterion for such foliations. 4. (T, 2008) Kovalev's theorem holds for the Assouad dimension on Hn. n n In other words, if E ⊂ H , dimA E < 1 then GQCdimA;H E = 0. Question: Kovalev's theorem in Hn for Hausdorff dimension? n n 3. For each s 2 [1; Q] 9 E ⊂ H compact s.t. GQCdimH E = dim E = s. 8 4. (T, 2008) Kovalev's theorem holds for the Assouad dimension on Hn. n n In other words, if E ⊂ H , dimA E < 1 then GQCdimA;H E = 0. Question: Kovalev's theorem in Hn for Hausdorff dimension? n n 3. For each s 2 [1; Q] 9 E ⊂ H compact s.t. GQCdimH E = dim E = s. Proof sketch: For s ≤ 2n + 1, choose E to be the union of line segments along integral curves of the horiz vector field X1 emanating from a Cantor set in the z2 ··· znt-subspace. Criteria of the Bourdon{Pansu theorem hold. S For 2n + 1 ≤ s ≤ Q, let E = r2C @BH (o; r) be a Cantor set's worth of Kor´anyi n spheres @BH (o; r) = fp 2 H : dH (o; p) = rg. Apply a version of the Bourdon{Pansu criterion for such foliations. 9 Question: Kovalev's theorem in Hn for Hausdorff dimension? n n 3. For each s 2 [1; Q] 9 E ⊂ H compact s.t. GQCdimH E = dim E = s. Proof sketch: For s ≤ 2n + 1, choose E to be the union of line segments along integral curves of the horiz vector field X1 emanating from a Cantor set in the z2 ··· znt-subspace. Criteria of the Bourdon{Pansu theorem hold. S For 2n + 1 ≤ s ≤ Q, let E = r2C @BH (o; r) be a Cantor set's worth of Kor´anyi n spheres @BH (o; r) = fp 2 H : dH (o; p) = rg. Apply a version of the Bourdon{Pansu criterion for such foliations. 4. (T, 2008) Kovalev's theorem holds for the Assouad dimension on Hn. n n In other words, if E ⊂ H , dimA E < 1 then GQCdimA;H E = 0. 10 n n 3. For each s 2 [1; Q] 9 E ⊂ H compact s.t. GQCdimH E = dim E = s. Proof sketch: For s ≤ 2n + 1, choose E to be the union of line segments along integral curves of the horiz vector field X1 emanating from a Cantor set in the z2 ··· znt-subspace. Criteria of the Bourdon{Pansu theorem hold. S For 2n + 1 ≤ s ≤ Q, let E = r2C @BH (o; r) be a Cantor set's worth of Kor´anyi n spheres @BH (o; r) = fp 2 H : dH (o; p) = rg. Apply a version of the Bourdon{Pansu criterion for such foliations. 4. (T, 2008) Kovalev's theorem holds for the Assouad dimension on Hn. n n In other words, if E ⊂ H , dimA E < 1 then GQCdimA;H E = 0. Question: Kovalev's theorem in Hn for Hausdorff dimension? 11 Examples: ' = 1, ' = xk , ' = yk , k = 1;:::; n generate left translation flows P ' = 2t V = 2tT + j (xj Xj + yj Yj ) generates dilation flow p0 7! δes (p0) Quasiconformal flows n Recall the standard left invariant vector fields X1; Y1;:::; Xn; Yn generating HH . @ @ @ @ Xj (p) = + 2yj ; Yj (p) = − 2xj @xj @t @yj @t Kor´anyiand Reimann (1995) give conditions on a vector field V which guarantee that the time s map p(0) 7! p(s) associated to the ODEp _ = V (p) is K(s)-qc. Basic structure is n 1 X V = ' T + (X ' Y − Y ' X ) for ' 2 C 1( n) 4 j j j j H j=1 with additional restrictions on the second horiz derivatives of '. 12 Quasiconformal flows n Recall the standard left invariant vector fields X1; Y1;:::; Xn; Yn generating HH . @ @ @ @ Xj (p) = + 2yj ; Yj (p) = − 2xj @xj @t @yj @t Kor´anyiand Reimann (1995) give conditions on a vector field V which guarantee that the time s map p(0) 7! p(s) associated to the ODEp _ = V (p) is K(s)-qc. Basic structure is n 1 X V = ' T + (X ' Y − Y ' X ) for ' 2 C 1( n) 4 j j j j H j=1 with additional restrictions on the second horiz derivatives of '. Examples: ' = 1, ' = xk , ' = yk , k = 1;:::; n generate left translation flows P ' = 2t V = 2tT + j (xj Xj + yj Yj ) generates dilation flow p0 7! δes (p0) 13 f Fix a ball B(p; R) and a family of disjoint balls Bj = B(pj ; rj ) ⊂ B(p; r). Choose potentials 'j generating contractive similarities with fixed points at the P pj , and define ' = j χj 'j for suitable smooth cutoff functions χj . For suitable s, the time s map F associated to ' is qc, fixes @B(p; r), and contracts each Bj . Moreover, F is conformal outside of B and inside each Bj . Iterate. As the flow method only works for smooth maps, use compactness of the space of normalized K-qc maps to pass to the limit. 14 In particular, it follows that f is a.e. diff'ble in horizontal directions, and that f is n n n a generalized contact map, dhfp = (Dfp)∗jHp H maps HpH to Hf (p)H a.e. Intuition: The CC ball at p of radius 0 < r 1 is comparable to the box [−r; r]2n × [−r 2; r 2], sheared so that the [−r; r]2n factor lies along the subspace n HpH . Metric quasiconformality ) at a point of differentiability, the size r and size r 2 directions cannot be interchanged by f .
Load more

Recommended publications
  • 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.
    [Show full text]
  • 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...............
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Graphs of Groups: Word Computations and Free Crossed Resolutions
    Graphs of Groups: Word Computations and Free Crossed Resolutions Emma Jane Moore November 2000 Summary i Acknowledgements I would like to thank my supervisors, Prof. Ronnie Brown and Dr. Chris Wensley, for their support and guidance over the past three years. I am also grateful to Prof. Tim Porter for helpful discussions on category theory. Many thanks to my family and friends for their support and encouragement and to all the staff and students at the School of Mathematics with whom I had the pleasure of working. Finally thanks to EPSRC who paid my fees and supported me financially. ii Contents Introduction 1 1 Groupoids 4 1.1 Graphs, Categories, and Groupoids .................... 4 1.1.1 Graphs ................................ 5 1.1.2 Categories and Groupoids ..................... 6 1.2 Groups to Groupoids ............................ 12 1.2.1 Examples and Properties of Groupoids .............. 12 1.2.2 Free Groupoid and Words ..................... 15 1.2.3 Normal Subgroupoids and Quotient Groupoids .......... 17 1.2.4 Groupoid Cosets and Transversals ................. 18 1.2.5 Universal Groupoids ........................ 20 1.2.6 Groupoid Pushouts and Presentations .............. 24 2 Graphs of Groups and Normal Forms 29 2.1 Fundamental Groupoid of a Graph of Groups .............. 29 2.1.1 Graph of Groups .......................... 30 2.1.2 Fundamental Groupoid ....................... 31 2.1.3 Fundamental Group ........................ 34 2.1.4 Normal Form ............................ 35 2.1.5 Examples .............................. 41 2.1.6 Graph of Groupoids ........................ 47 2.2 Implementation ............................... 49 2.2.1 Normal Form and Knuth Bendix Methods ............ 50 iii 2.2.2 Implementation and GAP4 Output ................ 54 3 Total Groupoids and Total Spaces 61 3.1 Cylinders .................................
    [Show full text]
  • Regular Representations and Coset Representations Combined with a Mirror-Permutation
    MATCH MATCH Commun. Math. Comput. Chem. 83 (2020) 65-84 Communications in Mathematical and in Computer Chemistry ISSN 0340 - 6253 Regular Representations and Coset Representations Combined with a Mirror-Permutation. Concordant Construction of the Mark Table and the USCI-CF Table of the Point Group Td Shinsaku Fujita Shonan Institute of Chemoinformatics and Mathematical Chemistry, Kaneko 479-7 Ooimachi, Ashigara-Kami-Gun, Kanagawa-Ken, 258-0019 Japan [email protected] (Received November 21, 2018) Abstract A combined-permutation representation (CPR) of degree 26 (= 24 + 2) for a regular representation (RR) of degree 24 is derived algebraically from a multiplica- tion table of the point group Td, where reflections are explicitly considered in the form of a mirror-permutation of degree 2. Thereby, the standard mark table and the standard USCI-CF table (unit-subduced-cycle-index-with-chirality-fittingness table) are concordantly generated by using the GAP functions MarkTableforUSCI and constructUSCITable, which have been developed by Fujita for the purpose of systematizing the concordant construction. A CPR for each coset representation (CR) (Gin)Td is obtained algebraically by means of the GAP function CosetRepCF developed by Fujita (Appendix A). On the other hand, CPRs for CRs are obtained geometrically as permutation groups by considering appropriate skeletons, where the point group Td acts on an orbit of jTdj=jGij positions to be equivalent in a given skeleton so as to generate the CPR of degree jTdj=jGij. An RR as a CPR is obtained by considering a regular body (RB), the jTdj positions of which are considered to be governed by RR (C1n)Td.
    [Show full text]
  • Affine Permutations and Rational Slope Parking Functions
    AFFINE PERMUTATIONS AND RATIONAL SLOPE PARKING FUNCTIONS EUGENE GORSKY, MIKHAIL MAZIN, AND MONICA VAZIRANI ABSTRACT. We introduce a new approach to the enumeration of rational slope parking functions with respect to the area and a generalized dinv statistics, and relate the combinatorics of parking functions to that of affine permutations. We relate our construction to two previously known combinatorial constructions: Haglund’s bijection ζ exchanging the pairs of statistics (area, dinv) and (bounce, area) on Dyck paths, and the Pak-Stanley labeling of the regions of k-Shi hyperplane arrangements by k-parking functions. Essentially, our approach can be viewed as a generalization and a unification of these two constructions. We also relate our combinatorial constructions to representation theory. We derive new formulas for the Poincar´epolynomials of certain affine Springer fibers and describe a connection to the theory of finite dimensional representations of DAHA and nonsymmetric Macdonald polynomials. 1. INTRODUCTION Parking functions are ubiquitous in the modern combinatorics. There is a natural action of the symmetric group on parking functions, and the orbits are labeled by the non-decreasing parking functions which correspond natu- rally to the Dyck paths. This provides a link between parking functions and various combinatorial objects counted by Catalan numbers. In a series of papers Garsia, Haglund, Haiman, et al. [18, 19], related the combinatorics of Catalan numbers and parking functions to the space of diagonal harmonics. There are also deep connections to the geometry of the Hilbert scheme. Since the works of Pak and Stanley [29], Athanasiadis and Linusson [5] , it became clear that parking functions are tightly related to the combinatorics of the affine symmetric group.
    [Show full text]
  • Affine Symmetric Group Joel Brewster Lewis¹*
    WikiJournal of Science, 2021, 4(1):3 doi: 10.15347/wjs/2021.003 Encyclopedic Review Article Affine symmetric group Joel Brewster Lewis¹* Abstract The affine symmetric group is a mathematical structure that describes the symmetries of the number line and the regular triangular tesselation of the plane, as well as related higher dimensional objects. It is an infinite extension of the symmetric group, which consists of all permutations (rearrangements) of a finite set. In addition to its geo- metric description, the affine symmetric group may be defined as the collection of permutations of the integers (..., −2, −1, 0, 1, 2, ...) that are periodic in a certain sense, or in purely algebraic terms as a group with certain gen- erators and relations. These different definitions allow for the extension of many important properties of the finite symmetric group to the infinite setting, and are studied as part of the fields of combinatorics and representation theory. Definitions Non-technical summary The affine symmetric group, 푆̃푛, may be equivalently Flat, straight-edged shapes (like triangles) or 3D ones defined as an abstract group by generators and rela- (like pyramids) have only a finite number of symme- tions, or in terms of concrete geometric and combina- tries. In contrast, the affine symmetric group is a way to torial models. mathematically describe all the symmetries possible when an infinitely large flat surface is covered by trian- gular tiles. As with many subjects in mathematics, it can Algebraic definition also be thought of in a number of ways: for example, it In terms of generators and relations, 푆̃푛 is generated also describes the symmetries of the infinitely long by a set number line, or the possible arrangements of all inte- gers (..., −2, −1, 0, 1, 2, ...) with certain repetitive pat- 푠 , 푠 , … , 푠 0 1 푛−1 terns.
    [Show full text]
  • The Enumeration of Fully Commutative Affine Permutations
    The enumeration of fully commutative affine permutations Christopher R. H. Hanusa, Brant C. Jones To cite this version: Christopher R. H. Hanusa, Brant C. Jones. The enumeration of fully commutative affine permutations. 23rd International Conference on Formal Power Series and Algebraic Combinatorics (FPSAC 2011), 2011, Reykjavik, Iceland. pp.457-468. hal-01215077 HAL Id: hal-01215077 https://hal.inria.fr/hal-01215077 Submitted on 13 Oct 2015 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. FPSAC 2011, Reykjav´ık, Iceland DMTCS proc. AO, 2011, 457–468 The enumeration of fully commutative affine permutations Christopher R. H. Hanusa1yand Brant C. Jones2z 1Department of Mathematics, Queens College (CUNY), NY, USA 2Department of Mathematics and Statistics, James Madison University, Harrisonburg, VA, USA Abstract. We give a generating function for the fully commutative affine permutations enumerated by rank and Coxeter length, extending formulas due to Stembridge and Barcucci–Del Lungo–Pergola–Pinzani. For fixed rank, the length generating functions have coefficients that are periodic with period dividing the rank. In the course of proving these formulas, we obtain results that elucidate the structure of the fully commutative affine permutations.
    [Show full text]
  • 19. Automorphism Group of S Definition-Lemma 19.1. Let G Be A
    19. Automorphism group of Sn Definition-Lemma 19.1. Let G be a group. The automorphism group of G, denoted Aut(G), is the subgroup of A(Sn) of all automorphisms of G. Proof. We check that Aut(G) is closed under products and inverses. Suppose that φ and 2 Aut(G). Let ξ = φ ◦ . If g and h 2 G then ξ(gh) = (φ ◦ )(gh) = φ( (gh)) = φ( (g) (h)) = φ( (g))φ( (h)) = (φ ◦ )(g)(φ ◦ )(h) = ξ(g)ξ(h): Thus ξ = φ◦ is a group homomorphism. Thus Aut(G) is closed under products. Now let ξ = φ−1. If g and h 2 G then we can find g0 and h0 such that g = φ(g0) and h = φ(h0). It follows that ξ(gh) = ξ(φ(g0)φ(h0)) = ξ(φ(g0h0)) = g0h0 = ξ(g)ξ(h): Thus ξ = φ−1 is a group homomorphism. Thus Aut(G) is closed under inverses. Lemma 19.2. Let G be a group and let a 2 G. φa is the automorphism of G given by conjugation by a, φ(g) = aga−1. If a and b 2 G then φab = φaφb: Proof. Both sides are functions from G to G. We just need to check that they have the same effect on any element g of G: (φa ◦ φb)(g) = φa(φb(g)) −1 = φa(bgb ) = a(bgb−1)a−1 = (ab)g(ab)−1 = φab(g): 1 Definition-Lemma 19.3. We say that an automorphism φ of G is inner if φ = φa for some a.
    [Show full text]
  • The Affine Group I. Bruhat Decomposition*
    CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 20, 512-539 (1972) The Affine Group I. Bruhat Decomposition* LOUIS SOLOMON Department of Mathematics, University of Wisconsin, Madison, Wisconsin 53706 Received March 22,1971 TO PROFESSOR RICHARD BRAUER, TO COMMEMORATE HIS SEVENTIETH BIRTHDAY, FEBRUARY 10, 1971 1. INTRODUCTION Let G be a finite group with (B, N) pair. Iwahori [6, 7] has shown that the double coset algebra defined by the subgroup B of G has a set Sl , ... , Sn of distinguished generators and an irreducible character sgn of degree one such that sgn(Si) = -1 for i = 1, ... , n. The double centralizer theory sets up a one to one correspondence between irreducible characters of the double coset algebra and irreducible characters of G which appear in the permutation character afforded by G/B. In particular, sgn corresponds to the Steinberg character of G. It seems [11, Theorem 1] that the existence of the sgn character is a general fact of combinatorics. One can associate with a finite incidence structure E an associative algebra C [11] which has a set Y1 , ... , Yn of distinguished generators. Under mild hypotheses, C has a character of degree one, called sgn, such that sgn(Yi) = -1 for i = 1, ... , n. In case E is the Tits geometry [13] or building defined by a finite group G with (B, N) pair, Iwahori's work shows that C is isomorphic to the double coset algebra [4, 12] defined by the subgroup B of G. Under this isomorphism Yi corresponds to Si' In this paper we study the same circle of ideas in case E is affine geometry of dimension n over a finite field K = Fq • We shall see that C is isomorphic to the double coset algebra defined by a certain subgroup B of the affine group G.
    [Show full text]