spectra and assembly in algebraic l theory andrew ranicki
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SPECTRA AND ASSEMBLY IN ALGEBRAIC L-THEORY Andrew Ranicki - PowerPoint PPT Presentation

1 SPECTRA AND ASSEMBLY IN ALGEBRAIC L-THEORY Andrew Ranicki (Edinburgh) http://www.maths.ed.ac.uk/ aar Max Planck Institute for Mathematics, Bonn 3rd December, 2012 2 What are spectra, assembly and algebraic L -theory doing in geometric


  1. 1 SPECTRA AND ASSEMBLY IN ALGEBRAIC L-THEORY Andrew Ranicki (Edinburgh) http://www.maths.ed.ac.uk/ � aar Max Planck Institute for Mathematics, Bonn 3rd December, 2012

  2. 2 What are spectra, assembly and algebraic L -theory doing in geometric topology? ◮ Answer: they are useful homotopy theoretic and algebraic tools in understanding the homotopy types of topological manifolds. ◮ Surgery theory thrives on these tools! Especially in dimensions � = 3 , 4: would be good to know how to include 3 and 4. ◮ Spectra = stable homotopy theory ◮ Assembly = passage from local to global. ◮ Algebraic L -theory = quadratic forms, as in the Wall obstruction groups L ∗ ( Z [ π ]) for surgery on manifolds with fundamental group π .

  3. 3 A brief history of assembly ◮ Congress shall make no law . . . abridging . . . the right of the people to peaceable assembly First Amendment to the United States Constitution, 1791 ◮ Wall (1970) Surgery obstruction groups L ∗ ( Z [ π ]). Assembly modulo 2-torsion. ◮ Quinn (1971) Geometric L -theory assembly [ X , G / TOP ] → L n ( Z [ π 1 ( X )]) ◮ Ranicki (1979, 1992) Algebraic L -theory assembly A : H n ( X ; L • ) → L n ( Z [ π 1 ( X )]) ◮ Ranicki-Weiss (1990) Chain complexes and assembly ◮ Weiss-Williams (1995) Assembly via stable homotopy theory ◮ Davis-L¨ uck (1998) Assembly via equivariant homotopy theory ◮ Hambleton-Pedersen (2004) Identification of various assembly maps ◮ Applications of assembly to Novikov, Borel, Farrell-Jones,Baum-Connes conjectures, in many contexts besides algebraic L -theory, such as algebraic K -theory or K -theory of C ∗ -algebras. L¨ uck 2010 ICM talk.

  4. 4 Surgery theory ◮ The 1960’s saw a great flowering of the topology of high-dimensional manifolds, especially in dimensions > 4. ◮ The Browder-Novikov-Sullivan-Wall surgery theory combined with the Kirby-Siebenmann structure theory for topological manifolds provided construction methods for recognizing the homotopy types of topological manifolds among spaces with Poincar´ e duality. ◮ The spectra , assembly and L -theory of the title are the technical tools from homotopy theory and the algebraic theory of quadratic forms which are used to recognize topological manifolds in homotopy theory. ◮ Recognition only works in dimension > 4. Need much more subtle methods in dimensions 3 , 4.

  5. 5 Geometric Poincar´ e complexes ◮ An n -dimensional geometric Poincar´ e complex X is a finite CW complex together with a homology class [ X ] ∈ H n ( X ) such that there are induced Poincar´ e duality isomorphisms with arbitrary coefficients [ X ] ∩ − : H ∗ ( X ) ∼ = H n −∗ ( X ) . ◮ An n -dimensional topological manifold M is an n -dimensional geometric Poincar´ e complex for n � = 4, and for n = 4 is at least homotopy equivalent to a 4-dimensional Poincar´ e complex. ◮ Any finite CW complex homotopy equivalent to an n -dimensional topological manifold is a geometric Poincar´ e complex. ◮ When is an n -dimensional Poincar´ e complex X homotopy equivalent to an n -dimensional topological manifold? ◮ Motivational answer: for n > 4 if and only if the Mishchenko-R. symmetric signature σ ( X ) ∈ L n ( Z [ π 1 ( X )]) is in the image of the symmetric L -theory assembly map A : H n ( X ; L • ) → L n ( Z [ π 1 ( X )]).

  6. 6 Proto-assembly, from homotopy to homology ◮ A homology class [ X ] ∈ H n ( X ) is local in nature, depending only on the images [ X ] x ∈ H n ( X , X \{ x } ) ( x ∈ X ) . ◮ A map of spaces f : X → Y induces a chain map f ∗ : C ( X ) → C ( Y ). ◮ The proto-assembly function H 0 ( Y X ) → H 0 (Hom Z ( C ( X ) , C ( Y ))) ; f �→ f ∗ sends the homotopy class of a map f : X → Y to the chain homotopy class of f ∗ . ◮ Local to global. ◮ Vietoris theorem : if f : X → Y is a surjection of reasonable spaces (e.g. simplicial complexes) with acyclic point inverses H ∗ ( f − 1 ( x )) ∼ = H ∗ ( x ) ( x ∈ X ) then the proto-assembly f ∗ is an isomorphism in homology. ◮ More about this in Spiros Adams-Florou’s talk tomorrow.

  7. 7 Proto-assembly: the diagonal map ◮ The diagonal map ∆ : X → X × X ; x �→ ( x , x ) sends [ X ] ∈ H n ( X ) to the chain homotopy class ∆[ X ] ∈ H n ( X × X ) = H 0 (Hom Z ( C ( X ) n −∗ , C ( X ))) of the chain map ∆[ X ] = [ X ] ∩ − : C ( X ) n −∗ → C ( X ). Local to global. ◮ If X is a closed oriented n -dimensional manifold with fundamental class [ X ] ∈ H n ( X ) then � Z for r = n , generated by [ X ] x = 1 H r ( X , X \{ x } ) = 0 for r � = n . ◮ The local Poincar´ e duality isomorphisms [ X ] x ∩ − : H ∗ ( { x } ) ∼ = H n −∗ ( X , X \{ x } ( x ∈ X )) assemble to the global Poincar´ e duality isomorphisms : H ∗ ( X ) ∼ [ X ] ∩ = H n −∗ ( X ) .

  8. 8 Suspension and loop spaces ◮ Only really need Ω-spectra, but suspension spectra motivational. ◮ The suspension of a pointed space X is Σ X = S 1 ∧ X . ◮ The loop space of X is Ω X = X S 1 . ◮ Adjointness property: for any pointed X , Y X Σ Y = (Ω X ) Y , [Σ Y , X ] = [ Y , Ω X ] . ◮ In particular, for Y = S n have π n +1 ( X ) = π n (Ω X ) .

  9. 9 Suspension spectra ◮ A suspension spectrum is a sequence of pointed spaces and maps E = { E k , Σ E k → E k +1 | k � 0 } ◮ The homotopy groups of E are defined by π n ( E ) = lim π n + k ( E k ) . − → k ◮ Example The homology groups of a space X are the homotopy groups of the Eilenberg-MacLane suspension spectrum H ( X ) H n ( X ) = π n ( H ( X )) , H ( X ) k = X + ∧ K ( Z , k ) with X + = X ⊔ { + } . ◮ Hard to see the local nature of H ∗ ( X ).

  10. 10 The Pontrjagin-Thom transversality construction ◮ Given an oriented k -plane bundle η : X → BSO ( k ) let T ( η ) be the Thom space. ◮ Pontrjagin-Thom construction : Every map ρ : N n + k → T ( η ) from an oriented ( n + k )-dimensional manifold N is homotopic to a map transverse regular at the zero section X ⊂ T ( η ). The inverse image is an oriented n -dimensional submanifold M n = ρ − 1 ( X ) ⊂ N . ◮ The normal bundle of M ⊂ N is the pullback oriented k -plane bundle ν M ⊂ N = f ∗ η : M → X → BSO ( k ) of η along the restriction f = ρ | : M → X .

  11. 11 The Pontrjagin-Thom assembly in bordism theory ◮ The Thom space MSO ( k ) = T (1 k ) of the universal k -plane bundle 1 k : BSO ( k ) → BSO ( k ) is the k th space of the universal Thom suspension spectrum MSO = { MSO ( k ) | Σ MSO ( k ) → MSO ( k + 1) } . ◮ Let Ω SO n ( X ) be the bordism groups of closed oriented n -dimensional manifolds M n with a map M → X ◮ The Pontrjagin-Thom isomorphism π n ( X + ∧ MSO ) → Ω SO n ( X ) ; ( ρ : S n + k → X + ∧ MSO ( k )) �→ ( ρ | : M n = ρ − 1 ( X × BSO ( k )) → X ) will serve as a model for the algebraic L -theory assembly map A , but it is hard to see it as local to global. The Pontrjagin-Thom construction is too analytic to translate into algebra directly. Also, A is not in general an isomorphism.

  12. 12 Ω -spectra ◮ An Ω -spectrum is a sequence of pointed spaces and homotopy equivalences F = { F k , F k ≃ Ω F k − 1 | k ∈ Z } so that there are homotopy equivalences F 0 ≃ Ω F − 1 ≃ . . . ≃ Ω k F − k . ◮ The homotopy groups of F are defined by π n ( F ) = π n ( F 0 ) = . . . = π n + k ( F − k ) . ◮ There is no essential difference between the homotopy theoretic properties of the suspension spectra and Ω-spectra. ◮ A suspension spectrum E = { E k , Σ E k → E k +1 } determines an Ω-spectrum Ω ∞ E = F with the same homotopy groups Ω j E j − k , π n ( F ) = π n ( E ) . F = { F k ≃ Ω F k +1 } , F k = lim − → j

  13. 13 Homotopy invariant functors ◮ The homotopy groups of a covariant functor F : { topological spaces } → { Ω-spectra } ; X �→ F ( X ) are written F n ( X ) = π n ( F ( X )) ( n ∈ Z ) . ◮ F is homotopy invariant if for a homotopy equivalence X → Y , or equivalently there are induced isomorphisms ∼ = � F ∗ ( Y ) . F ∗ ( X ) ◮ The relative homotopy groups of a pair ( Y , X ⊆ Y ) F n ( Y , X ) = π n ( F ( Y ) / F ( X )) fit into the usual exact sequence · · · → F n ( X ) → F n ( Y ) → F n ( Y , X ) → F n − 1 ( X ) → . . . .

  14. 14 Generalized homology theories ◮ The functor F : { topological spaces } → { Ω-spectra } ; X �→ F ( X ) is excisive if for X = X 1 ∪ Y X 2 the inclusion ( X 1 , Y ) ⊂ ( X , X 2 ) induces excision isomorphisms ∼ = � F n ( X 1 , Y ) F n ( X , X 2 ) and there is defined a Mayer-Vietoris exact sequence · · · → F n ( Y ) → F n ( X 1 ) ⊕ F n ( X 2 ) → F n ( X ) → F n − 1 ( Y ) → . . . . ◮ F is a generalized homology functor if it is both homotopy invariant and excisive. ◮ The homotopy groups F ∗ ( X ) = π ∗ ( F ( X )) are called generalized homology groups .

  15. 15 Generalized homology functors and Ω -spectra I. ◮ Theorem (G.W. Whitehead 1962) An Ω-spectrum F = { F k , Ω F k ≃ F k − 1 | k ∈ Z } determines a generalized homology functor F = H (?; F ) : { topological spaces } → { Ω-spectra } ; X �→ F ( X ) = H ( X ; F ) = X + ∧ F . ◮ The generalized homology groups are π n + k ( X + ∧ F − k ) . H n ( X ; F ) = F n ( X ) = lim − → k ◮ Moreover, every generalized homology theory arises in this way.

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