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The leafwise Laplacian and its spectrum: the singular case Iakovos Androulidakis Department of Mathematics, University of Athens Bialoweiza, June 2012 I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case


  1. The leafwise Laplacian and its spectrum: the singular case Iakovos Androulidakis Department of Mathematics, University of Athens Bialoweiza, June 2012 I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 1 / 25

  2. Summary Introduction 1 Foliations and Laplacians Statement of 3 theorems How to prove these theorems 2 The C ∗ -algebra of a foliation Pseudodifferential calculus Proofs The singular case 3 Almost regular foliations Stefan-Sussmann foliations Generalizations: Singular foliations 4 I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 2 / 25

  3. Introduction Foliations and Laplacians 1.1 Definition: Foliation Partition to connected submanifolds. Local picture: I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 3 / 25

  4. Introduction Foliations and Laplacians 1.1 Definition: Foliation Partition to connected submanifolds. Local picture: In other words: There is an open cover of M by foliation charts of the form Ω = U × T , where U ⊆ R p and T ⊆ R q . T is the transverse direction and U is the longitudinal or leafwise direction. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 3 / 25

  5. Introduction Foliations and Laplacians 1.1 Definition: Foliation Partition to connected submanifolds. Local picture: In other words: There is an open cover of M by foliation charts of the form Ω = U × T , where U ⊆ R p and T ⊆ R q . T is the transverse direction and U is the longitudinal or leafwise direction. The change of charts is of the form f ( u , t ) = ( g ( u , t ) , h ( t )) . I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 3 / 25

  6. Introduction Foliations and Laplacians 1.1 Laplacians Each leaf is a complete Riemannian manifold: Laplacian ∆ L acting on L 2 ( L ) The family of leafwise Laplacians: Laplacian ∆ M acting on L 2 ( M ) I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 4 / 25

  7. Introduction Statement of 3 theorems Statement of 3 theorems Theorem 1 (Connes, Kordyukov) ∆ M and ∆ L are essentially self-adjoint. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 5 / 25

  8. Introduction Statement of 3 theorems Statement of 3 theorems Theorem 1 (Connes, Kordyukov) ∆ M and ∆ L are essentially self-adjoint. Also true (and more interesting) for ∆ M + f , ∆ L + f where f is a smooth function on M . more generally for every leafwise elliptic (pseudo-)differential operator. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 5 / 25

  9. Introduction Statement of 3 theorems Statement of 3 theorems Theorem 1 (Connes, Kordyukov) ∆ M and ∆ L are essentially self-adjoint. Also true (and more interesting) for ∆ M + f , ∆ L + f where f is a smooth function on M . more generally for every leafwise elliptic (pseudo-)differential operator. Not trivial because: ∆ M not elliptic (as an operator on M ). L not compact. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 5 / 25

  10. Introduction Statement of 3 theorems Spectrum of the Laplacian Theorem 2 (Kordyukov) If L is dense + amenability assumptions, ∆ M and ∆ L have the same spec- trum. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 6 / 25

  11. Introduction Statement of 3 theorems Spectrum of the Laplacian Theorem 2 (Kordyukov) If L is dense + amenability assumptions, ∆ M and ∆ L have the same spec- trum. Theorem 3 (Connes) In many cases, one can predict the possible gaps in the spectrum. The same is true for all leafwise elliptic operators. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 6 / 25

  12. How to prove these theorems The C ∗ -algebra of a foliation 2.1 The C ∗ -algebra Main tool: The foliation C ∗ -algebra C ∗ ( M , F ) . Its construction: Completion of a convolution algebra I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 7 / 25

  13. How to prove these theorems The C ∗ -algebra of a foliation 2.1 The C ∗ -algebra Main tool: The foliation C ∗ -algebra C ∗ ( M , F ) . Its construction: Completion of a convolution algebra � Kernels k ( x , y ) : k 1 ∗ k 2 = k 1 ( x , z ) k 2 ( z , y ) dz Case of a single leaf: ( x , y ) ∈ M × M � C ∗ ( M , F ) = K ( L 2 ( M )) Take any I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 7 / 25

  14. How to prove these theorems The C ∗ -algebra of a foliation 2.1 The C ∗ -algebra Main tool: The foliation C ∗ -algebra C ∗ ( M , F ) . Its construction: Completion of a convolution algebra � Kernels k ( x , y ) : k 1 ∗ k 2 = k 1 ( x , z ) k 2 ( z , y ) dz Case of a single leaf: ( x , y ) ∈ M × M � C ∗ ( M , F ) = K ( L 2 ( M )) Take any a product, a fibre bundle p : M → B : ( x , y ) ∈ M × M s.t. p ( x ) = p ( y ) � C ∗ ( M , F ) = C ( B ) ⊗ K Take I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 7 / 25

  15. How to prove these theorems The C ∗ -algebra of a foliation 2.1 The C ∗ -algebra Main tool: The foliation C ∗ -algebra C ∗ ( M , F ) . Its construction: Completion of a convolution algebra � Kernels k ( x , y ) : k 1 ∗ k 2 = k 1 ( x , z ) k 2 ( z , y ) dz Case of a single leaf: ( x , y ) ∈ M × M � C ∗ ( M , F ) = K ( L 2 ( M )) Take any a product, a fibre bundle p : M → B : ( x , y ) ∈ M × M s.t. p ( x ) = p ( y ) � C ∗ ( M , F ) = C ( B ) ⊗ K Take General case: ( x , y ) ∈ M × M s.t. x , y in same leaf L ; γ path on L connecting x , y ; h γ path holonomy depends only on homotopy class of γ H ( F ) = { ( x , germ ( h γ ) , y ) } Holonomy groupoid. topology, manifold structure ⇒ H ( F ) is a Lie groupoid (not always Hausdorff). I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 7 / 25

  16. How to prove these theorems The C ∗ -algebra of a foliation 2.1 The C ∗ -algebra Main tool: The foliation C ∗ -algebra C ∗ ( M , F ) . Its construction: Completion of a convolution algebra � Kernels k ( x , y ) : k 1 ∗ k 2 = k 1 ( x , z ) k 2 ( z , y ) dz Case of a single leaf: ( x , y ) ∈ M × M � C ∗ ( M , F ) = K ( L 2 ( M )) Take any a product, a fibre bundle p : M → B : ( x , y ) ∈ M × M s.t. p ( x ) = p ( y ) � C ∗ ( M , F ) = C ( B ) ⊗ K Take General case: ( x , y ) ∈ M × M s.t. x , y in same leaf L ; γ path on L connecting x , y ; h γ path holonomy depends only on homotopy class of γ H ( F ) = { ( x , germ ( h γ ) , y ) } Holonomy groupoid. topology, manifold structure ⇒ H ( F ) is a Lie groupoid (not always Hausdorff). C ∗ ( M , F ) = continuous functions on ”space of leaves M/F ”. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 7 / 25

  17. How to prove these theorems Pseudodifferential calculus 2.2 Pseudodifferential operators (Connes) The Lie algebra of vector fields tangent to the foliation acts by unbounded multipliers on C ∞ c ( G ) . The algebra generated is the algebra of differential operators. I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 8 / 25

  18. How to prove these theorems Pseudodifferential calculus 2.2 Pseudodifferential operators (Connes) The Lie algebra of vector fields tangent to the foliation acts by unbounded multipliers on C ∞ c ( G ) . The algebra generated is the algebra of differential operators. Using Fourier transform one can write a differential operator P (acting by left multiplication on f ∈ C ∞ c ( G ) ) as: � ( Pf )( x , y ) = exp ( i � φ ( x , z ) , ξ � ) α ( x , ξ ) χ ( x , z ) f ( z , y ) dξdz Where I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 8 / 25

  19. How to prove these theorems Pseudodifferential calculus 2.2 Pseudodifferential operators (Connes) The Lie algebra of vector fields tangent to the foliation acts by unbounded multipliers on C ∞ c ( G ) . The algebra generated is the algebra of differential operators. Using Fourier transform one can write a differential operator P (acting by left multiplication on f ∈ C ∞ c ( G ) ) as: � ( Pf )( x , y ) = exp ( i � φ ( x , z ) , ξ � ) α ( x , ξ ) χ ( x , z ) f ( z , y ) dξdz Where φ is the phase: through a local diffeomorphism defined on an open subset � Ω ≃ U × U × T ⊂ G (where Ω = U × T is a foliation chart). φ ( x , z ) = x − z ∈ F x ; χ is the cut-off function: χ smooth, χ ( x , x ) = 1 on (a compact subset ∈ � of) Ω , χ ( x , z ) = 0 for ( x , z ) / Ω ; α ∈ C ∞ ( F ∗ ) is a polynomial on ξ . It is called the symbol of P . I. Androulidakis (Athens) The leafwise Laplacian and its spectrum: the singular case Bialoweiza, June 2012 8 / 25

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