NONCOMMUTATIVE LOCALIZATION IN ALGEBRA AND TOPOLOGY Andrew Ranicki (Edinburgh) aar. Heidelberg, 17th December, 2008
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1 1 NONCOMMUTATIVE LOCALIZATION IN ALGEBRA AND TOPOLOGY Andrew Ranicki (Edinburgh) aar Heidelberg, 17th December, 2008
2 Noncommutative localization Localizations of noncommutative rings such as group rings Z[π] are rings with complicated properties in algebra and interesting applications to topology. The applications are to spaces X with infinite fundamental group π 1 (X ), e.g. amalgamated free products and HNN extensions, such as occur when X is a knot or link complement. The surgery classification of high-dimensional manifolds and Poincaré complexes, finite domination, fibre bundles over S 1, open books, circle-valued Morse theory, Morse theory of closed 1-forms, rational Novikov homology, codimension 1 and 2 splitting, homology surgery, knots and links. High-dimensional knot theory, Springer (1998) Survey: e-print AT in Noncommutative localization in algebra and topology, LMS Lecture Notes 330, Cambridge University Press (2006) 2
3 3 The cobordism/concordance groups of boundary links An n-dimensional µ-component boundary link is a link l : µ S n S n+2 such that there exists a µ-component Seifert surface M n+1 = µ i=1 M i S n+2 with M = l( µ S n ) S n+2. Boundary condition equivalent to the existence of a surjection π 1 (S n+2 \l( µ S n )) F µ sending the µ meridians to µ generators of the free group F µ of rank µ. Let C n (F µ ) be the cobordism group of n-dimensional µ-component boundary links. A 1-component boundary link is a knot k : S n S n+2, and C n (F 1 ) = C n is the knot cobordism group. Problem Compute C n (F µ )!
4 A 2-component boundary link l : S 1 S 1 S 3 4
5 5 Brief history of the knot cobordism groups C (Fox-Milnor 1957) Definition of C 1. (Kervaire 1966) Definition of C for > 1 and C 2 = 0. (Levine 1969) C = C +4 for > 1. Computation of C 2 +1 for > 0, using Seifert forms over Z, S 1 Z = Q and signatures C 2 +1 = Z Z 2 Z 4. (Kearton 1975) Expression of C 2 +1 for > 0, using a commutative localization S 1 Z[z, z 1 ] and S 1 Z[z, z 1 ]/Z[z, z 1 ]-valued Blanchfield forms. (Casson-Gordon 1976) ker(c 1 C 5 ) 0 using commutative localization. (Cochran-Orr-Teichner 2003) Near-computation of C 1, using noncommutative Ore localization of group rings and L 2 -signatures.
6 Brief history of the boundary link cobordism groups C (F µ ) (Cappell-Shaneson 1980) Geometric expression of C (F µ ) for > 1 as relative Γ-groups, and C 2 (F µ ) = 0. (Duval 1984) Algebraic expression of C 2 +1 (F µ ) for > 0, using a noncommutative localization Σ 1 Z[F µ ] and Σ 1 Z[F µ ]/Z[F µ ]-valued Blanchfield forms. (Ko 1989) Algebraic expression of C 2 +1 (F µ ) for > 0, using Seifert forms over Z[F µ ]. (Sheiham 2003) Computation of C 2 +1 (F µ ) for > 0, using noncommutative signatures C 2 +1 (F µ ) = Z Z 2 Z 4 Wishful thinking Compute C 1 (F µ ) for µ > 1 using noncommutative localization. Z 8. 6
7 7 Alexander duality in H and H but not in π 1 Want to investigate knotting properties of submanifolds N n M m, especially in codimension m n = 2, using the complement P = M\N. Alexander duality for H, H. The homology and cohomology of M, N, P are related by Z-module isomorphisms H (M, P) = H m (N), H (M, P) = H m (N). Failure of Alexander duality for π 1. The group morphisms π 1 (P) π 1 (M) induced by P M are isomorphisms for n m 3, but not in general for n m = 1 or 2. The Z[π 1 (P)]-module homology H ( P) of the universal cover P depends on the knotting of N M, whereas the Z-module homology H (P) does not.
8 8 Change of rings For a ring A let Mod(A) be the category of left A-modules. Given a ring morphism φ : A B regard B as a (B, A)-bimodule by B B A B ; (b, x, a) b.x.φ(a). Use this to define the change of rings a functor φ = B A : Mod(A) Mod(B) ; M B A M. An A-module chain complex C is B-contractible if the B-module chain complex B A C is contractible.
9 9 Knotting and unknotting Slogan The fundamental group π 1 detects knotting for n m = 1 or 2, whereas Z-coefficient homology and cohomology do not. The applications of algebraic K- and L-theory to knots and links use the chain complexes of the universal covers of the complements. They involve the algebraic K- and L-theory of B-contractible A-module chain complexes for augmentations φ = ɛ : A = Z[π 1 ] B = Z ; n g g g. g π 1 g π 1 In favourable circumstances (e.g. π 1 = F µ ) there exists a stably flat noncommutative localization A Σ 1 A such that an A-module chain complex C is B-contractible if and only if C is Σ 1 A-contractible. The algebraic K- and L-theory of such C can be then described entirely in terms of A.
10 Algebraic K-theory I. Let A be an associative ring with 1. The projective class group K 0 (A) is the abelian group with one generator [P] for each isomorphism class of f.g. projective A-modules P, and relations [P Q] = [P] + [Q] K 0 (A). A finite f.g. projective A-module chain complex C has a chain homotopy invariant projective class [C] = ( ) i [C i ] K 0 (A). i=0 Example K 0 (Z) = Z. The projective class of a finite f.g. free A-module chain complex is just the Euler characteristic the projective class [C] = χ(c) = ( ) i dim A (C i ) im(k 0 (Z) K 0 (A)). i=0 10
11 11 Algebraic K-theory II. The Whitehead group K 1 (A) is the abelian group with one generator τ(f ) for each automorphism f : P P of a f.g. projective A-module P, and relations τ(f f ) = τ(f ) + τ(f ), τ(gfg 1 ) = τ(f ) K 1 (A). The Whitehead torsion of a contractible finite based f.g. free A-module chain complex C is τ(c) = τ(d + Γ : C odd C even ) K 1 (A) with Γ : 0 1 : C C any chain contraction dγ + Γd = 1 : C r C r. Can generalize K 0 (A), K 1 (A) to K (A) for all Z.
12 Change of rings in algebraic K-theory 12 A ring morphism φ : A B induces an exact sequence of algebraic K-groups K n (A) φ K n (B) K n (φ) K n 1 (A)... A B-contractible finite f.g. free A-module chain complex C with χ(c) = 0 Z has a Reidemeister torsion τ[c] ker(k 1 (φ) K 0 (A)) = im(k 1 (B) K 1 (φ)) = coker(φ : K 1 (A) K 1 (B)) given by τ(b A C) K 1 (B) for any choice of bases for C. (Milnor 1966) Whitehead torsion interpretation of the Reidemeister torsion of a knot using the augmentation φ : A = Z[z, z 1 ] B = F for any field F.
13 13 Commutative localization The localization of a commutative ring A inverting a multiplicatively closed subset S A of non-zero divisors with 1 S is the ring S 1 A of fractions a/s (a A, s S), where a/s = b/t if and only if at = bs. Usual addition and multiplication a/s + b/t = (at + bs)/(st), (a/s)(b/t) = (as)/(bt) and canonical embedding A S 1 A; a a/1. For an integral domain A and S = A {0} S 1 A = quotient field(a). Example If A = Z then S 1 A = Q.
14 The standard example k : S n S n+2 I. The exterior of an n-dimensional knot k is an (n + 2)-dimensional manifold with boundary (X, X ) = (cl.(s n+2 \(k(s n ) D 2 )), S n S 1 ) with X S n+2 \S n a deformation retract of the complement. The generator 1 H 1 (X ) = Z is realized by a homology equivalence (f, f ) : (X, X ) (X 0, X 0 ) with (X 0, X 0 ) the exterior of the trivial knot k 0 : S n S n+2 = S n D 2 D n+1 S 1 with X 0 = D n+1 S 1 S 1, and f a homeomorphism. Theorem (Dehn+P. for n = 1, Kervaire+Levine for n 2) k is unknotted if and only if f is a homotopy equivalence. The circle S 1 has universal cover S 1 = R, with π 1 (S 1 ) = Z, Z[π 1 (S 1 )] = Z[z, z 1 ]. The homology equivalence f : X S 1 lifts to a Z-equivariant map f : X R with X = f R the pullback infinite cyclic cover of X. 14
15 The standard example k : S n S n+2 II. The Blanchfield localization S 1 A of A = Z[z, z 1 ] inverts S = ɛ 1 (1) A, with ɛ : A Z; z 1 the augmentation. The cellular A-module chain map f : C(X ) C(R) induces a chain equivalence f = 1 f : Z A C(X ) = C(X ) Z A C(R) = C(S 1 ). The algebraic mapping cone C = C(f ) is a finite f.g. free A-module chain complex such that H (Z A C) = 0, S 1 H (C) = 0, χ(c) = 0. The Reidemeister torsion is an isotopy invariant τ[c] = (1 φ(z))/ (k) K 1 (φ) = coker(φ : K 1 (A) K 1 (S 1 A)) = (S 1 A) /A with (k) S the Alexander polynomial of k. The localization φ : A S 1 A first used by Blanchfield (1957) in the study of the duality properties of H (X ). 15
16 The noncommutative Ore localization 16 (Ore 1931) The Ore localization S 1 A is defined for a multiplicatively closed subset S A with 1 S, and such that for all a A, s S there exist b A, t S with ta = bs A. E.g. central, sa = as for all a A, s S. The Ore localization is the ring of fractions S 1 A = (S A)/, with (s, a) (t, b) if and only if there exist u, v A with us = vt S, ua = vb A. An element of S 1 A is a noncommutative fraction s 1 a = equivalence class of (s, a) S 1 A with addition and multiplication more or less as usual. Example A commutative localization is an Ore localization.
17 17 Ore localization is flat The Ore localization S 1 A is a flat A-module, i.e. the functor S 1 : Mod(A) Mod(S 1 A) ; M S 1 M = S 1 A A M is exact. For any A-module M Tor A i (S 1 A, M) = 0 (i 1). For any A-module chain complex C H (S 1 C) = S 1 H (C). Proposition For any finite f.g. free S 1 A-module chain complex D there exists a finite f.g. free A-module chain complex C with an S 1 A-module isomorphism S 1 C = D. Proof Clear denominators!
18 Universal localization I. 18 Given a ring A and a set Σ of elements, matrices, morphisms,..., it is possible to construct a new ring Σ 1 A, the localization of A inverting all the elements in Σ. In general, A and Σ 1 A are noncommutative, and A Σ 1 A is not injective. Original algebraic motivation: construction of noncommutative analogues of the quotient field of an integral domain. Topological applications to knots and links use the algebraic K- and L-theory of A and Σ 1 A, in two separate situations: Given a ring morphism φ : A B there exists a factorization φ : A Σ 1 A B such that a free A-module chain complex C is B-contractible if and only if C is Σ 1 A-contractible. If a ring R is an amalgamated free product or an HNN extension then for k = 2 or 3 the matrix ring M k (R) is Σ 1 A for a triangular matrix ring A M k (R) : gives all known decomposition theorems for K (R) and L (R).
19 19 Universal localization II. A = ring, Σ = a set of morphisms s : P Q of f.g. projective A-modules. A ring morphism A B is Σ-inverting if each 1 s : B A P B A Q (s Σ) is a B-module isomorphism. (P.M. Cohn 1970) The universal localization Σ 1 A is a ring with a Σ-inverting morphism A Σ 1 A such that any Σ-inverting morphism A B has a unique factorization A Σ 1 A B. The universal localization Σ 1 A exists (and it is unique); but it could be 0 e.g if 0 Σ. In general, Σ 1 A is not a flat A-module. Σ 1 A is a flat A-module if and only if Σ 1 A is an Ore localization (Beachy, Teichner, 2003).
20 The normal form I. 20 (Gerasimov, Malcolmson 1981) Assume Σ consists of all the morphisms s : P Q of f.g. projective A-modules such that 1 s : Σ 1 P Σ 1 Q is a Σ 1 A-module isomorphism. (Can enlarge any Σ to have this property). Every element x Σ 1 A is of the form x = fs 1 g for some (s : P Q) Σ, f : P A, g : A Q. For f.g. projective A-modules M, N every Σ 1 A-module morphism x : Σ 1 M Σ 1 N is of the form x = fs 1 g for some (s : P Q) Σ, f : P N, g : M Q M Addition by g P s Q f N. fs 1 g +f s 1 g = (f f )(s s ) 1 (g g ) : Σ 1 M Σ 1 N Similarly for composition.
21 The normal form II. For f.g. projective M, N, a Σ 1 A-module morphism fs 1 g : Σ 1 M Σ 1 N is such that fs 1 g = 0 if and only if there is a commutative diagram of A-module morphisms s 0 0 g 0 s s 2 g 2 f f P P 1 P 2 M ( p p1 p 2 m Q Q 1 Q 2 N ) ( q q1 q 2 n ) T L with s, s 1, s 2, ( p p 1 p 2 ), ( q q1 q 2 ) T Σ. (Exercise: diagram = fs 1 g = 0). 21
22 Localization in algebraic K-theory I. 22 Assume each (s : P Q) Σ is injective and A Σ 1 A is injective. The torsion exact category T (A, Σ) has objects A-modules T with Σ 1 T = 0, hom. dim. (T ) = 1. E.g., T = coker(s) for s Σ. Theorem (Bass 1968 for central, Schofield 1985 for universal Σ 1 A). Exact sequence K 1 (A) K 1 (Σ 1 A) K 0 (T (A, Σ)) K 0 (A) K 0 (Σ 1 A) with ( τ(fs 1 g : Σ 1 M Σ 1 N) ) = [ ( ) f 0 coker( : P M N Q) ] [ coker(s : P Q) ] s g Theorem (Quillen 1972, Grayson 1980) Higher K-theory localization exact sequence for Ore localization Σ 1 A, by flatness.
23 Universal localization is not flat 23 In general, if M is an A-module and C is an A-module chain complex Tor A (Σ 1 A, M) 0, H (Σ 1 C) Σ 1 H (C). True for Ore localization Σ 1 A, by flatness. Example The universal localization Σ 1 A of the free product A = Z x 1, x 2 = Z[x 1 ] Z[x 2 ] inverting Σ = {x 1 } is not flat. The 1-dimensional f.g. free A-module chain complex d C = (x 1 x 2 ) : C 1 = A A C 0 = A is a resolution of H 0 (C) = Z and H 1 (Σ 1 C) = Tor A 1 (Σ 1 A, H 0 (C)) = Σ 1 A Σ 1 H 1 (C) = 0.
24 24 Chain complex lifting I. A lift of a f.g. free Σ 1 A-module chain complex D is a f.g. projective A-module chain complex C with a chain equivalence Σ 1 C D. For an Ore localization Σ 1 A one can lift every n-dimensional f.g. free Σ 1 A-module chain complex D, for any n 0. For a universal localization Σ 1 A one can only lift for n 2 in general. Proposition (Neeman+R., 2001) For n 3 there are lifting obstructions in Tor A i (Σ 1 A, Σ 1 A) for i 2. Tor A 1 (Σ 1 A, Σ 1 A) = 0 always.
25 25 Chain complex lifting II. Example The boundary map in the Schofield exact sequence for an injective universal localization A Σ 1 A : K 1 (Σ 1 A) K 0 (T (A, Σ)) ; τ(d) [C] sends the Whitehead torsion τ(d) of a contractible based f.g. free Σ 1 A-module chain complex D to the projective class [C] of any f.g. projective A-module chain complex C such that Σ 1 C D.
26 26 Stable flatness A universal localization Σ 1 A is stably flat if Tor A i (Σ 1 A, Σ 1 A) = 0 (i 2). For stably flat Σ 1 A have stable exactness: H (Σ 1 C) = lim B Σ 1 H (B) with maps C B such that Σ 1 C Σ 1 B. Flat = stably flat. If Σ 1 A is flat (i.e. an Ore localization) then Tor A i (Σ 1 A, M) = 0 (i 1) for every A-module M. The special case M = Σ 1 A gives that Σ 1 A is stably flat.
27 A localization which is not stably flat Given a ring extension R S and an S-module M let K(M) = ker(s R M M). Theorem (Neeman, R. and Schofield) (i) The universal localization of the ring R 0 0 A = S R 0 = P 1 P 2 P 3 (columns) S S R inverting Σ = {P 3 P 2, P 2 P 1 } is Σ 1 A = M 3 (S). (ii) If S is a flat R-module then Tor A n 1(Σ 1 A, Σ 1 A) = M n (K n (S)) (n 3). (iii) If R is a field and dim R (S) = d then K n (S) = K(K(... K(S)... )) = R (d 1)nd. If d 2, e.g. S = R[x]/(x d ), then Σ 1 A is not stably flat. (e-print RA , Math. Proc. Camb. Phil. Soc. 2004). 27
28 28 Localization in algebraic K-theory II. Theorem (Neeman + R., 2001) If A Σ 1 A is injective and stably flat then : fibration sequence of exact categories T (A, Σ) P(A) P(Σ 1 A) with P(A) the category of f.g. projective A-modules, and every finite f.g. free Σ 1 A-module chain complex can be lifted, there are exact localization sequences K n (A) K n (Σ 1 A) K n 1 (T (A, Σ)) K n 1 (A)... e-print RA , Geometry and Topology (2004)
29 The standard example l : µ S n S n+2 I. 29 The exterior of an n-dimensional boundary link l is an (n + 2)-dimensional manifold with boundary (X, X ) = (cl.(s n+2 \((l( µ S n ) D 2 )), S n S 1 ) with X S n+2 \S n a deformation retract of the complement. (Cappell-Shaneson 1980) There is a homology equivalence (f, f ) : (X, X ) (X 0, X 0 ) with (X 0, X 0 ) the exterior of the trivial boundary link l 0 X 0 = #(S D n+1 ) µ S 1 µ 1 S n+1 µ π 1 (X 0 ) = F µ, and f a homeomorphism. The universal F µ -cover X 0 of X 0 and the pullback cover X = f X0 are such that f lifts to an F µ -equivariant map f : X X0 with C( f ) a Z-contractible f.g. free Z[F µ ]-module chain complex.
30 The standard example l : µ S n S n+2 II. The Blanchfield universal localization Σ 1 A of A = Z[F µ ] inverts the set Σ of all Z-invertible square matrices in A. (Sontag-Dicks 1978, Farber-Vogel 1986) Σ 1 A is stably flat. (R.-Sheiham 2003-) The algebraic mapping cone C = C( f ) is a finite f.g. free A-module chain complex such that H (Σ 1 C) = 0, giving an isotopy invariant τ[c] = 1/ (l) K 1 (φ) = coker(φ : K 1 (A) K 1 (S 1 A)) K 0 (T (A, Σ)) with (l) Σ the Alexander matrix of l. Isotopy invariant: mild generalization of the noncommutative Alexander polynomials of Farber (1986) and Garoufalidis-Kricker (2003). (R.-S.) Blanchfield and Seifert algebra in high-dimensional boundary link theory I. Algebraic K-theory, e-print AT , Geometry and Topology (2006) 30
31 31 Algebraic L-theory Let A be an associative ring with 1, and with an involution A A; a ā used to identify left A-modules = right A-modules. Example A group ring A = Z[π] with ḡ = g 1 for g π. The algebraic L-group L n (A) is the abelian group of cobordism classes (C, ψ) of n-dimensional f.g. projective A-module chain complexes C with an n-dimensional quadratic Poincaré duality ψ : H n (C) = H (C). These are the Wall (1970) surgery obstruction groups L (A), originally defined using quadratic forms and their automorphisms.
32 Localization in algebraic L-theory 32 Theorem (R for Ore, Vogel 1982 in general) For any injective universal localization A Σ 1 A of a ring with involution A there is an exact sequence of algebraic L-groups L n (A) L n (Σ 1 A) L n (A, Σ) L n 1 (A)... with L n (A, Σ) the cobordism group of Σ 1 A-contractible (n 1)-dimensional quadratic Poincaré complexes (C, ψ) over A. Corollary (Duval R. 2008) For n 2 the cobordism class of a boundary link l : µ S n S n+2 is the cobordism class of the Z-contractible (n + 2)-dimensional quadratic Poincaré complex (C( f ), ψ) over Z[F µ ] l = (C( f ), ψ) C n (F µ ) = L n+3 (Z[F µ ], Σ) with f : X X 0 the homology equivalence between the exteriors of l and l 0.
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