Spectral Triples on the Sierpinski Gasket

Transcription

1 Spectral Triples on the Sierpinski Gasket Fabio Cipriani Dipartimento di Matematica Politecnico di Milano - Italy ( Joint works with D. Guido, T. Isola, J.-L. Sauvageot ) AMS Meeting "Analysis, Probability and Mathematical Physics on Fractals" Cornell University Ithaca NY, September, 10th to 13th, 2011

2 Sierpinski gasket K C and its Dirichlet form (E, F) Duomo di Amalfi: Chiostro, sec. XIII The aim of the work is to construct Spectral Triples (A, D, H) able to describe the geometric features of K such as: Dimension, Topology, Volume, Distance and Energy. Our constructions rely on two facts: the Dirichlet space F C(K), domain of the Dirichlet form (E, F) of the standard Laplacian on K, is a semisimple Banach -algebra so that its K-theory coincides with the K theory of C(K) and with the K-theory of K [F.C. Pacific J. (2006)] the traces of finite energy functions a F on K to boundary of lacunas l σ K belong to fractional Sobolev spaces H α (l σ) [A. Jonsson Math. Z. (2005)]

3 Novelty with respect to [Christensen-Ivan-Schrohe arxiv: (2010)] is that the Dirichlet form can be recovered E[a] = const.trace ω ( [D, a] 2 D δ D ) a F a new energy dimension δ D := 2 of the energy functionals ln 5/3 ln 2 appears as the abscissa of convergence C s Trace, ( [D, a] 2 D s ) a F The difference w.r.t. the Hausdorff dimension is a consequence of the equivalent facts δ D d H = ln 3 ln 2 Volume and Energy are distributed singularly on K [M. Hino Prob Th. Rel. Fields (2005)] there are no nontrivial algebras in the domain of the Laplacian

4 Spectral Triples (Connes 1985) The notion of Spectral Triple abstracts some basic properties of a Dirac operator on a complete Riemannian manifold and lies at the foundation of a metric geometry in generalized settings, where the algebra of coordinates of the space maybe commutative or not. A Spectral Triple (A, H, D) over a C -algebra A B(H), consists of a smooth sub- algebra A A and a self-adjoint operator (D, dom (D)) on H subject to: [D, a] is a bounded operator for all a A a(i + D 2 ) 1/2 is a compact operator on H for all a A In the framework of the Sierpinski gasket K A := C(K) is the commutative C -algebra of continuous functions A := F is the domain of the Dirichlet form (E, F) of the standard Laplacian.

5 Parity, Summability and Dimensional Spectrum of Spectral Triples A Spectral Triple is called even if there exists γ B(H) such that γ 2 = I, γ = γ, γd + Dγ = 0, γa = aγ, a A a Spectral Triple is called finitely p-summable, for some p 1, if a(i + D 2 ) 1/2 L p (H) a Spectral Triple is called (d, )-summable if a(i + D 2 ) d/2 L (1, ) (H) a p-summable Spectral Triple has dicrete spectrum if there exists a discrete set F C such that all zeta functions associated to elements a A ζ a D : {z C : Re z p} C ζ a D(s) := Tr (a D s ) extends to meromorphic functions with poles contained in F. The dimensional spectrum of (A, H, D) is defined to be the smallest of such sets.

6 Example: Canonical Spectral Triple of a Riemannian manifold M H := L 2 (Λ(M)) be the Hilbert space of square integrable sections of the exterior bundle of differential forms considered as a module over A := C 0(M) D := d + d is the first order differential (Dirac) operator whose square is the Hodge-de Rham Laplacian HdR = dd + d d of M a(i + D 2 ) 1/2 is a compact by Sobolev embeddings for all a A := C c norm of commutators coincides with Lipschiz semi-norms [D, a] = da the Riemannian distance may be recovered from commutators as d(x, y) := sup{a(x) a(y) : a A, [D, a] 1} the Minakshisundaram-Pleijel asymptotic of the heat semigroup e t HdR as t 0 allows to identify the dimensional spectrum with {0, 1,, dim M} C so that the spectral triple is (dim M, )-summable. (M)

7 Fredholm modules (Athiyah (1969), Kasparov (1975)) Fredholm modules on C -algebras generalize elliptic operators on manifolds: A Fredholm modules (F, H) over a C -algebra A B(H), consists of a symmetry F B(H): F = F, F 2 = I such that [F, a] is compact for all a A FM lie at the core of Noncommutative Geometry of A. Connes where the compact operator da := i[f, a] is the operator theoretic substitute for the differential of a A FM has been constructed on p.c.f. fractals by [C.-Sauvageot CMP (2009)] and on more general fractals by [Ionescu-Rogers-Teplyaev (2011)] Proposition. (Connes (1986), Baaj-Julg (1983)) The sign F := sign(d) of the Dirac operator of a Spectral Triple (A, H, D) gives rise to a Fredholm module (F, H).

8 Pairing with K-theory and an Index Theorem on SG Modifying the proof of the Connes Index Theorem for FM [Connes (1986)], to take into account that Dirac operators on SG have dim Ker (D) = +, it is possible to construct topological invariants. Theorem. (CGIS 2010) The Spectral Triples on SG determine a group homomorphism on the K-theory ch D : K 1(F) C which is integer valued ch D(K 1(F)) Z. These values are the index of suitable Fredholm operators: for all invertible u GL (F), setting P := (I + F)/2, the operator G u := PuP is Fredholm and ch D[u] = Index (G u) = 1 2 2m+1 Trace (u[f, u 1 ] 2m+1 ) m 1. These values can be interpreted as winding numbers around lacunas in SG.

9 Quasi-circles We will need to consider on the 1-torus T = {z C : z = 1} structures of quasi-circle associated to the following Dirichlet forms and their associated Spectral Triples for any α (0, 1). Lemma. Fractional Dirichlet forms on a circle (CGIS 2010) Consider the Dirichlet form on L 2 (T) defined on the fractional Sobolev space E α[a] := ϕ α(z w) a(z) a(w) 2 dzdw F α := {a L 2 (T) : E α[a] < + } T T where ϕ α is the Clausen cosine function for 0 < α 1. Then H α := L 2 (T T) is a symmetric Hilbert C(K)-bimodule w.r.t. actions and involutions given by (aξ)(z, w) := a(z)ξ(z, w), (ξa)(z, w) := ξ(z, w)a(w), (J ξ)(z, w) := ξ(w, z). The derivation α : F α H α associated to E α is given by α(a)(z, w) := ϕ α(z w)(a(z) a(w)).

10 Proposition. Spectral Triples on a circle (CGIS 2010) Consider on the Hilbert space K α := L 2 (T T) L 2 (T), the left C(T)-module structure resulting from the sum of those of L 2 (T T) and L 2 (T) and the operator ( ) 0 α D α := α. 0 a(z) a(w) 2 z w 2α+1 < + } is a uniformly dense Then A α := {a C(T) : sup z T T subalgebra of C(T) and (A α, D α, K α) is a densely defined Spectral Triple on C(T). The dimensional spectrum is { 1 }. α

11 Dirac operators on K. Identifying isometrically the main lacuna l of the gasket with the circle T, consider the Dirac operator (C(K), D, K ) where K := L 2 (l l ) L 2 (l ) D := D α the action of C(K) is given by restriction π (a)b := a l. Fix γ > 0 and for σ consider the Dirac operators (C(K), π σ, D σ, K σ) where K σ := K D σ := 2 γ σ D α the action of C(K) is given by contraction/restriction π σ(a)b := (a F σ) l b. Finally, consider the Dirac operator (C(K), π, D, K) where K := σ K σ π := σ π σ D := σ D σ Notice that dim Ker D = + and that D 1 will be defined to be zero on Ker D.

12 Volume functionals and their Spectral dimensions Theorem. (CGIS 2010) The zeta function Z D of the Dirac operator (C(K), D, K), i.e. the meromorphic extension of the function C s Trace( D s ) is given by Z D(s) = 4 z(αs) 1 3c s where z denotes the Riemann zeta function. The dimensional spectrum is given by S dim = { 1 α } { ln 3 ln 2 γ 1( 1 + 2πi ln 3 k ) : k Z} and the abscissa of convergence is d D = max(α 1, ln 3 ln 2 γ 1 ). When 0 < γ < ln 3 α ln 2 there is a simple pole in d D = ln 3 ln 2 γ 1 and the residue of the meromorphic extension of C s Trace(f D s ) gives the Hausdorff measure of dimension d H = ln 3 ln 2 Trace Dix(f D s ) = Res s=dd Trace(f D s ) = 4d z(d) f dµ. ln 3 (2π) d Notice the complex dimensions and the independence of the residue Hausdorff measure upon γ > 0. K

13 Spectral Triples and Connes metrics on the Sierpinski gasket Theorem. (CGIS 2010) (C(K), D, K) is a Spectral Triple for any 0 < γ 1. In particular the seminorm a [D, a] is a Lip-seminorm in the sense of Rieffel so that the distance it determines induces the original topology on K. If α < γ this distance is bi-lipschitz w.r.t. the power (ρ geo) γ.

14 Energy functionals and their Spectral dimensions By the Spectral Triple it is possible to recover, in addition to dimension, volume measure and metric, also the energy form of K Theorem. (CGIS 2010) Consider the Spectral Triple (C(K), D, K) for α α 0 := ln 5 ( 1 ln 3 1) 0, 87 ln 4 2 ln 2 and assume a F. Then the abscissa of convergence of C s Trace( [D, a] 2 D s ) is δ D := max(α 1 1 ln 5/3, 2 γ ). ln 2 If δ D > α 1 then s = δ D is a simple pole and the residue is proportional to the Dirichlet form Res s=δd Trace( [D, a] 2 D s ) = const. E[a] a F ;

15 The (γ, α)-plane Above the line α = γ/d S, the volume measure is a multiple of the Hausdorff measure H ds where d S = ln 3 and the spectral dimension is ln 2 dd = d S γ in the square 0 < α, γ 1, (A, D, H) is a Spectral Triple whose Fredholm module has nontrivial pairing with all generators of the K-theory K 1 (K) and "generates" the K-homology K 0 (K) below the line α = γ, the distance ρ D is bi-lipschitz with (ρ geo) γ in the strip α < α 0 < γ < 1 and above the hyperbola αδ D(γ) = 1 the energy functional is proportional to the Dirichlet form, where δ D(γ) = 2 ln(5/3) ln 2 ln γ 1 is the energy dimension.