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Blowups, deformations to normal cones and Lie groupoids (joint work - PowerPoint PPT Presentation

Blowups, deformations to normal cones and Lie groupoids (joint work with Claire Debord) Claire Debord & GS: Blowup constructions for Lie groupoids and a Boutet de Monvel type calculus (In preparation) Georges Skandalis Universit e


  1. Blowups, deformations to normal cones and Lie groupoids (joint work with Claire Debord) Claire Debord & GS: Blowup constructions for Lie groupoids and a Boutet de Monvel type calculus (In preparation) Georges Skandalis Universit´ e Paris-Diderot Paris 7 Institut de Math´ ematiques de Jussieu Paris Rive Gauche May 29, 2017 Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 1 / 24

  2. A geometric idea A Lie groupoid G ◆ M gives a family of longitudinal di ff erential operators (its algebroid). Evolution along the groupoid. V ⇢ M a submanifold, seen as an obstacle. It forces operators to “slow down” near V in the normal direction. Propagation should preserve V and move along a subgroupoid Γ ◆ V . We propose a construction of a Lie groupoid taking into account this kind of propagation. The plan of this talk: Present two general constructions of groupoids: 1 Deformation to the normal cone ( DNC ) 2 Blowup ( Blup ). Compute, connecting maps and index elements arising in these constructions. Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 2 / 24

  3. Two classical constructions 1. The Deformation to the Normal Cone Let V be an immersed submanifold of a smooth manifold M with normal bundle N M V . The deformation to the normal cone is DNC ( M, V ) = M ⇥ R ⇤ t N M V ⇥ { 0 } . Smooth structure, generated by the following maps to be smooth ( x 2 M , � 2 R ⇤ , y 2 V , ⇠ 2 T y M/T y V ): p : DNC ( M, V ) ! M ⇥ R : p ( x, � ) = ( x, � ) , p ( y, ⇠ , 0) = ( y, 0); given f : M ! R , smooth with f | V = 0, f ( x, � ) = f ( x ) ˜ ˜ , ˜ f : DNC ( M, V ) ! R , f ( y, ⇠ , 0) = ( d f ) y ( ⇠ ) � Remark. Restricts to every (locally closed) subset of R . + t N M Define DNC + ( M, V ) = M ⇥ R ⇤ V ⇥ { 0 } . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 3 / 24

  4. / ✏ Functoriality of DNC Consider a commutative diagram of smooth maps V �  M f V ✏ f M V 0 �  / M 0 Horizontal arrows are immersions of submanifolds. We get a smooth map DNC ( f ) : DNC ( M, V ) ! DNC ( M 0 , V 0 ) defined by ⇢ DNC ( f )( x, � ) = ( f M ( x ) , � ) for x 2 M, � 2 R ⇤ for x 2 V, ¯ DNC ( f )( x, ⇠ , 0) = ( f V ( x ) , ( d f ) x ( ⇠ ) , 0) ⇠ 2 T x M/T x V f ) x : T x M/T x V ! T f V ( x ) M 0 /T f V ( x ) V 0 is the map induced by ( d where ( d f M ) x . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 4 / 24

  5. Deformation groupoid Let Γ be a subgroupoid and an immersed submanifold of a Lie groupoid r,s ◆ G (0) . G By functoriality DNC ( G, Γ ) ◆ DNC ( G (0) , Γ (0) ) is naturally a Lie groupoid: source and range maps are DNC ( s ) and DNC ( r ); space of composable arrows (identifies with) DNC ( G (2) , Γ (2) ) and its product with DNC ( m ) ( m : G (2) ! G i is the product). i Remark Γ is a groupoid over N G (0) Γ ◆ N G (0) N G Γ (0) denoted N G Γ (0) . Γ ⇥ { 0 } ◆ ( G (0) ⇥ R ⇤ ) t N G (0) DNC ( G, Γ ) = ( G ⇥ R ⇤ ) t N G Γ (0) ⇥ { 0 } Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 5 / 24

  6. Examples of DNC groupoids 1 Tangent groupoid of Alain Connes DNC ( M ⇥ M, ∆ M ) = ( M ⇥ M ) ⇥ R ⇤ t TM ⇥ { 0 } . Adiabatic groupoid ( [Monthubert-Pierrot 99, Nistor-Weinstein-Xu 99] ): restriction of DNC ( G, G (0) ) over G (0) ⇥ [0 , 1]. This groupoid encodes the index of M , of G . 2 V submanifold of G (0) , saturated for G , DNC ( G, G V V ) normal groupoid of immersion G V ! G which gives the shriek map [Hilsum-S 87] . V , 3 K maximal compact subgroup of a Lie group G , DNC ( G, K ) used by Higson to recover “Dirac induction”. 4 Double deformation: G 1 ⇢ G 2 ⇢ G 3 . � � DNC 2 ( G 3 , G 2 , G 1 ) = DNC DNC ( G 3 , G 1 ) , DNC ( G 2 , G 1 ) . Example: ⇡ : E ! M a submersion; consider ∆ E ⇢ E ⇥ M E ⇢ E ⇥ E : Used by [Debord-Lescure-Nistor] for a diagram chasing proof of the Atiyah-Singer index theorem ( E ! M is the normal bundle). ... Many more... Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 6 / 24

  7. 2. The Blowup construction V ⇢ M closed submanifold. Scaling action of R ⇤ on M ⇥ R ⇤ extends to the gauge action on DNC ( M, V ) = M ⇥ R ⇤ t N M V : DNC ( M, V ) ⇥ R ⇤ � ! DNC ( M, V ) ( z, t, � ) 7! ( z, � t ) for t 6 = 0 ( x, 1 ( x, X, 0 , � ) 7! λ X, 0) for t = 0 The manifold V ⇥ R embeds in DNC ( M, V ). The gauge action is free and proper on the open subset DNC ( M, V ) \ V ⇥ R of DNC ( M, V ). We let: � � / R ⇤ = M \ V t P ( N M Blup ( M, V ) = DNC ( M, V ) \ V ⇥ R V ) . Put also � � + = M \ V t S ( N M DNC + ( M, V ) \ V ⇥ R + / R ⇤ SBlup ( M, V ) = V ) . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 7 / 24

  8. ✏ / Fonctoriality of Blup V �  gives DNC ( f ) : DNC ( M, V ) ! DNC ( M 0 , V 0 ) M f V ✏ f M V 0 �  / M 0 Equivariant under the gauge action: it passes to the quotient Blup ... where it is defined. Let U f ( M, V ) = DNC ( M, V ) \ DNC ( f ) � 1 ( V 0 ⇥ R ); define Blup f ( M, V ) = U f / R ⇤ ⇢ Blup ( M, V ) Then, by passing DNC ( f ) to the quotient: Blup ( f ) : Blup f ( M, V ) ! Blup ( M 0 , V 0 ) Analogous construction SBlup ( f ) : SBlup f ( M, V ) ! SBlup ( M 0 , V 0 ). Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 8 / 24

  9. Blowup groupoid r,s ◆ G (0) . Define Let Γ be a closed Lie subgroupoid of a Lie groupoid G ^ DNC ( G, Γ ) = U r ( G, Γ ) \ U s ( G, Γ ) elements whose image by DNC ( s ) and DNC ( r ) are not in Γ (0) ⇥ R . Subgroupoid of DNC ( G, Γ ). Gauge action: groupoid automorphisms, whence (or by functoriality) DNC ( G, Γ ) / R ⇤ ◆ Blup ( G (0) , Γ (0) ) ^ Blup r,s ( G, Γ ) = is naturally a Lie groupoid; source = Blup ( s ), range = Blup ( r ) and product = Blup ( m ). Analogous constructions hold for SBlup . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 9 / 24

  10. Examples of blowup groupoids Let V ⇢ M be a hypersurface. G b = SBlup r,s ( M ⇥ M, V ⇥ V ) ⇢ SBlup ( M ⇥ M, V ⇥ V ) | {z } | {z } The b-calculus groupoid Melrose’s b-space G 0 = SBlup r,s ( M ⇥ M, ∆ ( V )) ⇢ SBlup ( M ⇥ M, ∆ ( V )) | {z } | {z } Mazzeo-Melrose’s 0-space The 0-calculus groupoid Can take a groupoid G ◆ M transverse to V . G b = SBlup r,s ( G, G V V )) and G 0 = SBlup r,s ( G, V ) . M = V ⇥ R , corresponding G 0 : Gauge adiabatic groupoid [Debord, S] . Remarks Iterate these constructions: manifolds with corners [Monthubert]. Also by iteration stratified manifolds [Debord, Lescure, Rochon]. Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 10 / 24

  11. VB -groupoids [Pradines] Lie groupoids E, Γ . Vector bundle structure p : E ! Γ . p is a groupoid morphism; all the groupoid maps for E are linear bundle maps. E (0) ⇢ E | Γ (0) subbundle; r E : E x ! E (0) r Γ ( x ) and s E : E x ! E (0) s Γ ( x ) , inverse: E x ! E x � 1 linear (for all x 2 Γ ) . product: { ( u, v ) 2 E x ⇥ E y ; s E ( u ) = r E ( v ) } ! E x · y linear for ( x, y ) 2 Γ (2) . With a VB -groupoid p : ( E, r E , s E ) ! ( Γ , r Γ , s Γ ) are associated: The projective VB -groupoid. P ( E ) = ( E \ (ker r [ ker s )) / R ⇤ ; The spherical VB -groupoid. P ( E ) = ( E \ (ker r [ ker s )) / R ⇤ + . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 11 / 24

  12. The case Γ =point: linear groupoids Suppose E is a (real) vector space and F ⇢ E a vector subspace. Let r, s : E ! F be two linear retractions. (Classical) facts 1 Unique linear groupoid structure on E : E ◆ F with source s , range r and units given by the inclusion F ⇢ E : Product u · v = u + v � s ( u ). Inverse of u is ( r + s � id )( u ). 2 E is the action groupoid E o r � s E/F . Remarks 1 This construction can be done with any field. 2 If r 6 = s , every orbit meets F \ { 0 } : the restriction ˚ E of E to F \ { 0 } is Morita equivalent to E . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 12 / 24

  13. The case Γ =point: linear groupoids Suppose E is a (real) vector space and F ⇢ E a vector subspace. Let r, s : E ! F be two linear retractions. (Classical) facts 1 Unique linear groupoid structure on E : E ◆ F with source s , range r and units given by the inclusion F ⇢ E : Product u · v = u + v � s ( u ). Inverse of u is ( r + s � id )( u ). 2 E is the action groupoid F o r � s E/F . Remarks 1 This construction can be done with any field. 2 If r 6 = s , every orbit meets F \ { 0 } : the restriction ˚ E of E to F \ { 0 } is Morita equivalent to E . In fact inclusion C ⇤ (˚ E ) ⇢ C ⇤ ( E ) isomorphism. ⇧ Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 12 / 24

  14. Projective and spherical groupoids Assume F 6 = { 0 } . The group R ⇤ acts freely on E \ (ker r [ ker s ) ◆ F \ V and leads to the projective groupoid: P E ◆ P ( F ). P E = P ( E ) \ P (ker r ) [ P (ker s ) Source and range are induced by s and r . For composable x , y 2 P E : x · y = { u + v � s ( u ) ; u 2 x, v 2 y ; s ( u ) = r ( v ) } and the inverse of x is ( s + r � id )( x ). The same for spherical... Remark If F is just a line, P E is a group: If r = s , then P E is isomorphic to the abelian group ker( r ) = ker( s ). If r 6 = s , then P E ' (ker( r ) \ ker( s )) o R ⇤ . Claire Debord and GS Blowps, DNC and Lie groupoids Toulouse 29/05/17 13 / 24

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