the topology of tiling spaces
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The Topology of Tiling Spaces Jean BELLISSARD 1 2 Georgia Institute - PowerPoint PPT Presentation

1 Bologna August 30th 2008 The Topology of Tiling Spaces Jean BELLISSARD 1 2 Georgia Institute of Technology, Atlanta, http://www.math.gatech.edu/ jeanbel/ Collaborations: R. BENEDETTI (U. Pisa, Italy) J.-M. GAMBAUDO (U. Nice, France)


  1. 1 Bologna August 30th 2008 The Topology of Tiling Spaces Jean BELLISSARD 1 2 Georgia Institute of Technology, Atlanta, http://www.math.gatech.edu/ ∼ jeanbel/ Collaborations: R. BENEDETTI (U. Pisa, Italy) J.-M. GAMBAUDO (U. Nice, France) D.J.L. HERRMANN (U. Tübingen, Germany) J. KELLENDONK (U. Lyon I, Lyon, France) J. SAVINIEN (Gatech, Atlanta, GA & U. Bielefeld, Germany) M. ZARROUATI (U. Toulouse III, Toulouse, France) 1 Georgia Institute of Technology, School of Mathematics, Atlanta, GA 30332-0160 2 e-mail: jeanbel@math.gatech.edu

  2. 2 Bologna August 30th 2008 Main References J. B  , The Gap Labeling Theorems for Schrödinger’s Operators , in From Number Theory to Physics , pp. 538-630, Les Houches March 89, Springer, J.M. Luck, P. Moussa & M. Waldschmidt Eds., (1993). J. K  , The local structure of tilings and their integer group of coinvariants , Comm. Math. Phys., 187 , (1997), 1823-1842. J. E. A  , I. P  , Topological invariants for substitution tilings and their associated C ∗ -algebras , Ergodic Theory Dynam. Systems, 18 , (1998), 509-537. A. H. F  , J. H  , The cohomology and K-theory of commuting homeomorphisms of the Cantor set , Ergodic Theory Dynam. Systems, 19 , (1999), 611-625. J. C. L  , Geometric models for quasicrystals I & II , Discrete Comput. Geom., 21 , (1999), 161-191 & 345-372.

  3. 3 Bologna August 30th 2008 J. B  , D. H  , M. Z  , Hull of Aperiodic Solids and Gap Labeling Theorems , In Directions in Mathematical Quasicrystals , CRM Monograph Series, Volume 13 , (2000), 207-259, M.B. Baake & R.V. Moody Eds., AMS Providence. L. S  , R. F. W  , Tiling spaces are Cantor set fiber bundles , Ergodic Theory Dynam. Systems, 23 , (2003), 307-316. J. B  , R. B  , J. M. G  , Spaces of Tilings, Finite Telescopic Approximations , Comm. Math. Phys., 261 , (2006), 1-41. J. B  , J. S  , A Spectral Sequence for the K-theory of Tiling Spaces , arXiv:0705.2483, submitted to Ergod. Th. Dyn. Syst., 2007.

  4. 4 Bologna August 30th 2008 Content 1. Tilings, Tilings... 2. The Hull as a Dynamical System 3. Branched Oriented Flat Riemannian Manifolds 4. Cohomology and K -Theory 5. Conclusion

  5. 5 Bologna August 30th 2008 I - Tilings, Tilings,...

  6. 6 Bologna August 30th 2008 - A triangle tiling -

  7. 7 Bologna August 30th 2008 - Dominos on a triangular lattice -

  8. 8 Bologna August 30th 2008 - Building the chair tiling -

  9. 9 Bologna August 30th 2008 - The chair tiling -

  10. 10 Bologna August 30th 2008 - The Penrose tiling -

  11. 11 Bologna August 30th 2008 - Kites and Darts -

  12. 12 Bologna August 30th 2008 - Rhombi in Penrose’s tiling -

  13. 13 Bologna August 30th 2008 - The Penrose tiling -

  14. 14 Bologna August 30th 2008 - The octagonal tiling -

  15. 15 Bologna August 30th 2008 - Octagonal tiling: inflation rules -

  16. 16 Bologna August 30th 2008 - Another octagonal tiling -

  17. 17 Bologna August 30th 2008 - Another octagonal tiling -

  18. 18 Bologna August 30th 2008 - Building the Pinwheel Tiling -

  19. 19 Bologna August 30th 2008 - The Pinwheel Tiling -

  20. 20 Bologna August 30th 2008 Aperiodic Materials 1. Periodic Crystals in d -dimensions: translation and crystal symmetries. Translation group T ≃ Z d . 2. Periodic Crystals in a Uniform Magnetic Field ; magnetic oscillations, Shubnikov-de Haas, de Haas-van Alfen. The magnetic field breaks the translation invariance to give some quasiperiodicity.

  21. 21 Bologna August 30th 2008 3. Quasicrystals : no translation symmetry, but icosahedral symmetry. Ex.: (a) Al 62 . 5 Cu 25 Fe 12 . 5 ; (b) Al 70 Pd 22 Mn 8 ; (c) Al 70 Pd 22 Re 8 ; 4. Disordered Media : random atomic positions (a) Normal metals (with defects or impurities); (b) Alloys (c) Doped semiconductors ( Si , AsGa , . . . );

  22. 22 Bologna August 30th 2008 - The icosahedral quasicrystal AlPdMn -

  23. 23 Bologna August 30th 2008 - The icosahedral quasicrystal HoMgZn -

  24. 24 Bologna August 30th 2008 II - The Hull as a Dynamical System

  25. 25 Bologna August 30th 2008 Point Sets A subset L ⊂ R d may be: 1. Discrete . 2. Uniformly discrete : ∃ r > 0 s.t. each ball of radius r contains at most one point of L . 3. Relatively dense : ∃ R > 0 s.t. each ball of radius R contains at least one points of L . 4. A Delone set: L is uniformly discrete and relatively dense. 5. Finite Local Complexity (FLC) : L − L is discrete and closed. 6. Meyer set: L and L − L are Delone.

  26. 26 Bologna August 30th 2008 Point Sets and Point Measures M ( R d ) is the set of Radon measures on R d namely the dual space to C c ( R d ) (continuous functions with compact support), endowed with the weak ∗ topology. For L a uniformly discrete point set in R d : ν : = ν L = � ∈ M ( R d ) . δ ( x − y ) y ∈L

  27. 27 Bologna August 30th 2008 Point Sets and Tilings Given a tiling with finitely many tiles (modulo translations) , a De- lone set is obtained by defining a point in the interior of each (translation equivalence class of) tile. Conversely, given a Delone set, a tiling is built through the Voronoi cells V ( x ) = { a ∈ R d ; | a − x | < | a − y | , ∀ y L \ { x }} 1. V ( x ) is an open convex polyhedron containing B ( x ; r ) and contained into B ( x ; R ). 2. Two Voronoi cells touch face-to-face. 3. If L is FLC , then the Voronoi tiling has finitely many tiles modulo transla- tions.

  28. 28 Bologna August 30th 2008 - Building a Voronoi cell-

  29. 29 Bologna August 30th 2008 - A Delone set and its Voronoi Tiling-

  30. 30 Bologna August 30th 2008 The Hull A point measure is µ ∈ M ( R d ) such that µ ( B ) ∈ N for any ball B ⊂ R d . Its support is 1. Discrete . 2. r-Uniformly discrete : i ff ∀ B ball of radius r , µ ( B ) ≤ 1. 3. R-Relatively dense : i ff for each ball B of radius R , µ ( B ) ≥ 1. R d acts on M ( R d ) by translation.

  31. 31 Bologna August 30th 2008 Theorem 1 The set of r-uniformly discrete point measures is compact and R d -invariant. Its subset of R-relatively dense measures is compact and R d -invariant. Definition 1 Given L a uniformly discrete subset of R d , the Hull of L is the closure in M ( R d ) of the R d -orbit of ν L . Hence the Hull is a compact metrizable space on which R d acts by homeomorphisms .

  32. 32 Bologna August 30th 2008 Properties of the Hull If L ⊂ R d is r -uniformly discrete with Hull Ω then using com- pactness 1. each point ω ∈ Ω is an r-uniformly discrete point measure with support L ω . 2. if L is ( r , R ) -Delone , so are all L ω ’s. 3. if, in addition, L is FLC , so are all the L ω ’s. Moreover then L − L = L ω − L ω ∀ ω ∈ Ω . Definition 2 The transversal of the Hull Ω of a uniformly discrete set is the set of ω ∈ Ω such that 0 ∈ L ω . Theorem 2 If L is FLC, then its transversal is completely discontinu- ous.

  33. 33 Bologna August 30th 2008 Local Isomorphism Classes and Tiling Space A patch is a finite subset of L of the form p = ( L − x ) ∩ B (0 , r 1 ) x ∈ L , r 1 ≥ 0 Given L a repetitive, FLC, Delone set let W be its set of finite patches: it is called the the L -dictionary . A Delone set (or a Tiling) L ′ is locally isomorphic to L if it has the same dictionary. The Tiling Space of L is the set of Local Isomorphism Classes of L . Theorem 3 The Tiling Space of L coincides with its Hull.

  34. 34 Bologna August 30th 2008 Minimality L is repetitive if for any finite patch p there is R > 0 such that each ball of radius R contains an ǫ -approximant of a translated of p . Theorem 4 R d acts minimaly on Ω if and only if L is repetitive.

  35. 35 Bologna August 30th 2008 Examples 1. Crystals : Ω = R d / T ≃ T d with the quotient action of R d on itself. (Here T is the translation group leaving the lattice invariant. T is isomorphic to Z D .) The transversal is a finite set (number of point per unit cell). 2. Impurities in Si : let L be the lattices sites for Si atoms (it is a Bravais lattice). Let A be a finite set (alphabet) indexing the types of impurities. The transversal is X = A Z d with Z d -action given by shifts. The Hull Ω is the mapping torus of X .

  36. 36 Bologna August 30th 2008 - The Hull of a Periodic Lattice -

  37. 37 Bologna August 30th 2008 Quasicrystals Use the cut-and-project construction: π � ←− R n π ⊥ R d ≃ E � −→ E ⊥ ≃ R n − d π � L π ⊥ ←− ˜ L −→ W , Here 1. ˜ L is a lattice in R n , 2. the window W is a compact polytope. 3. L is the quasilattice in E � defined as L = { π � ( m ) ∈ E � ; m ∈ ˜ L , π ⊥ ( m ) ∈ W }

  38. 38 Bologna August 30th 2008

  39. 39 Bologna August 30th 2008 - The transversal of the Octagonal Tiling is completely disconnected -

  40. 40 Bologna August 30th 2008 III - Branched Oriented Flat Riemannian Manifolds

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