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DYNAMICS, Geometry and Topology Dan Burghelea (and Stefan Haller) Department of mathematics Ohio State University, Columbuus, OH Goettingen, November, 2010 Author, Another Short Paper Title

DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

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Page 1: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

DYNAMICS, Geometry and Topology

Dan Burghelea (and Stefan Haller)

Department of mathematicsOhio State University, Columbuus, OH

Goettingen, November, 2010

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Page 2: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Prior work:

S. Smale, D.Fried, S.P.Novikov, A.V. Pajitnov,M. Hutchins- Y. J. Lee

Influential work :

E Witten, B.Hellfer - J.Sjöstrandt, T.Kato, M. Shubin

Work of Burghelea- Haller reported in this talk:1. Dynamics, Laplace transform and spectral geometry,Journal of Topology, No 1 20082. Torsion, as a function on the space of representations, inC*algebras and Elliptic Theory II, Trends in Mathematics, 20083. Papers in preparation

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Page 3: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

CONTENTS

Dynamics

Spectral geometry

Topology

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Page 4: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Dynamics = Smooth vector field X on a closed manifold M.

Elements of Dynamics=

Rest pointsVisible trajectories

1. Instantons,

2. Closed trajectories

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Page 5: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Under nondegeneracy hypothesis = Property G

1 The set of rest points is finite2 The set of instantons is at most countable,3 The set of closed trajectories is at most countable.

Theorem(Kupka -Smale) The set of vector fields which satisfy G isresidual in any Cr−topology

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Page 6: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

PROBLEM:Count rest points, instantons and closed trajectories,Relate the results of the counting to geometry andtopology,Provide new invariants for a vector field,

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Page 7: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Crash course in Dynamics

• M a smooth closed manifold

• X : M → TM a smooth vector field

• Ψt : M → M the flow of X a one parameter group ofdiffeomorphisms.

• θm(t) := Ψt (m) the trajectory with θm(0) = m.

• A parametrized trajectory θ : R→ M, is characterized by

dθ(t)/dt = X (θ(t) .

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Page 8: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

REST POINTS:

X := x ∈ M|X (x) = 0

For x ∈ X consider Dx (X ) : Tx (M)→ Tx (M)

the composition TxM Dx X→ Tx (TM)pr→ TxM.

• x ∈ X non degenerate= hyperbolic if

λ ∈ Spec Dx (X )⇒ <λ 6= 0.

• x ∈ X non degenerate⇒ has Morse index

indx = ]λ ∈ Spec Dx (X )|<λ > 0.

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Page 9: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

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Page 10: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

STABLE/UNSTABLE SET

for x ∈ X

W±x := y ∈ M| lim

t→±∞θx (t) = x

If x ∈ Xq then W±x are images of one to one immersions

W−x =im(i−x : Rq → M)

W +x =im(i−x : Rn−q → M)

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Page 11: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

>>

>

>

Red – Stable manifold Blue – Unstable manifold

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Page 12: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

TRAJECTORIES

• parametrized trajectory: θ : R→ M

• equivalency of parametrized trajectories: θ1 ≡ θ2iff θ1(t) = θ2(t + A) (for some A ∈ R)

• nonparametrized trajectory: is an equivalency class [θ] ofparametrized trajectories.

• instanton between two rest points x and y : is an Isolatednon parametrized trajectory [θ], with

limt→−∞ θ(t) = x and limt→∞ θ(t) = y

• closed trajectory : is a pair ˆ[θ] = ([θ],T ) s.t θ(t + T ) = θ(t).

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Page 13: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

^ ^^ ^ ^ ^

No Instantons

^ ^

^^

^^

Four Instantons

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Page 14: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Definition• An instanton [θ] (from x to y , x , y non degenerate rest points)is non degenerate if i−x t i+y along [θ], in which case

index x − index y = 1.

• Orientations ox and oy of the unstable manifolds W−x , and

W−y provide a sign

εox ,oy ([θ]) = ±1

For a closed trajectory ˆ[θ] = ([θ],T ) and m ∈ Γ, (Γ = θ(R),)consider:

Dm(ΨT ) : Tm(M)→ Tm(M) and

Dm(ΨT ) : Tm(M)/Tm(Γ)→ Tm(M)/Tm(Γ)

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Page 15: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

o(s) F(s, r -- 6 (s))

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Page 16: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Definition

The closed trajectory ˆ[θ] = ([θ],T ) is non degenerate iff

(Id − Dm(ΨT ))

is invertible; if soε([ ˆ[θ]]) := sign det(Id − DΨT (m))

p( ˆ[θ]) = sup k so that ˆ[θ] : S1 → M factors by a self mapof S1 of degree k .Assign to ˆ[θ] the rational number

ε( ˆ[θ])/p( ˆ[θ]) .

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Page 17: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Property G= H + MS + NCT

1 Property H: All rest points are hyperbolic.2 Property MS: For any two rest points x , y ∈ X i−x t i+y .3 Property NCT: All closed trajectories are nondegenerate.

Denote by :

C the set of closed trajectories andIx ,y the set of instantons from x to y .

For X satisfying G the sets C and Ix ,y are countable andnaturally filtered by finite sets

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Page 18: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Choose ξ ∈ H1(M; C) and ω ∈ Ω1(M),dω = 0 representing ξ.For a closed trajectory [θ] define the functions

Z ξ

[θ](z) :=

ε([θ])

p([θ])ez

R[θ] ξ

and for an instanton from x to y the function

Iox ,oy ,ω

[θ] (z) := εox ,oy ([θ])ezR[θ] ω

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Page 19: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

and then the formal power series

Z ξ(z) =∑

[θ]∈Cx,y

Z[θ](z)

Iox ,oy ,ω

[θ] (z) =∑

[θ]∈Ix,y

Iox ,oy[θ] (z)

WHEN THE SUMS DEFINED ABOVE ARE ACTUALLYHOLOMORPHIC FUNCTIONS?

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Page 20: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

A Riemannian metrics on M induces Riemannian metrics onW−

x if x nondegenerate. Denote by Bx (R) the ball of radius Rin W−

x .

DefinitionX satisfies (EG) (exponential growth property) if w.r. to some

(and then with any) Riemannian metric if Vol(Bx (R)) ≤ eCR

(for some C > 0).

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Page 21: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Definition

A closed 1-form ω ∈ Ω1(M) is called Lyapunov for X ifω(X )(m) ≤ 0 and ω(X )(m) = 0 only when m ∈ X .

A cohomology class [ω] is Lyapunov for X if it contains aclosed 1-form Lyapunov fo X .

X satisfies (L) (Lyapunov property)if the set of cohomologyclasses Lyapunov for X is nonempty.

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Page 22: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

TheoremSuppose X satisfies L and EG, ξ is a Lyapunov cohomologyclass for X and ω ∈ ξ. Choose a collection of orientations of theunstable manifolds O = ox , x ∈ X.

1. There exists ρ ∈ R so that the formal sums Z ξ(z) andIox ,oy ,ω

[θ] (z) are absolutely convergent for <z > ρ and defineholomorphic functions in z ∈ C|<z > ρ.

2. For any x ∈ Xk+1, z ∈ Xk−1 one has∑y∈Xk

IO,ωx ,y · IO,ωy ,z = 0.

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Page 23: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

A holomorphic family of cochain complexes

Suppose X satisfies G, L and EG. Define

C∗(M; X , ω)(z) := (C∗(M; X ), δ∗O,ω(z))

• Ck (M; X ) := Maps(Xk ,C)

• δ∗O,ω(z) : C∗(M; X )→ C∗+1(M; X ))

(δkO,ω(z)(f ))(u) :=

∑v∈X

IO,ωu,v (z)f (v)

This is a holomorphic family of cochain complexes with a base.

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Page 24: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

• If ω1 and ω2 represent ξ ∈ H1(M; R), O1 and O2 are two setsof orientations, there exists a canonical isomorphism between

(C∗(M; X ), δ∗O1,ω1(z)) and (C∗(M; X ), δ∗O2,ω2

(z)).

⇒ C∗(M; X , ξ)(z)

• The cohomology changes in dimension at finitely many z.

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Page 25: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Riemannian geometry

M closed manifoldX smooth vector field satisfying Gω Lyapunov closed one form for X

There exists g Riemannian metric so that X = −gradgω

Introduce Witten deformation (Ω∗M,dω(z) = d + zω ∧ · · · )equipped with the scalar products on Ω(M) defined by g. Whenz is a real number It Induces Laplacians

∆ωq (z) : Ω∗(M)→ Ω∗(M) = ∆q + z(LX + L∗X ) + z2|gradgω|2

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Page 26: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

One can show that for <z > ρ

Exactly nk eigenvalues of ∆ωk (z) go to zero exponentially

fast while the remaining have real part go to∞ linearly fastas <z →∞. As a consequenceOne has a canonical orthogonal decomposition

(Ω∗(M); dω(z)) := (Ω∗(M)sm(M),dω(z))⊕(Ω∗(M)la(M),dω(z))

which diagonalizes ∆ω∗ (z) = ∆sm

∗ (z)⊕∆la∗ (z).

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Page 27: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Theorem1. The above decomposition has an analytic continuation in theneighborhood of [0,∞).

If in addition X satisfies EG then:

2. For <z > ρ the Integration of differential forms on unstablemanifolds is well defined and provides an isomorpfism from(Ω∗(M)sm; dω(z)) to (C∗(M; X ), δ∗O1,ω1

(z)). The isomorphism iscanonical.

3. For <z > ρ large the (Ω∗(M)la; dω(z)) is acyclic and

log Tla(M,g, ω)(z)− Z X ,[ω](z) = zR(g,X , ω)

where Tla(M,g, ω)(z)is the complex Ray Singer torsion andR(g,X , ω) a numerical invariant defined below.

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Page 28: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Other invariants

X vector field which satisfies L with nk rest points of index k ona Riemannian manifold (M,g).

Consider∆X

q (z) : Ω∗(M)→ Ω∗(M) = ∆q + z(LX + L∗X ) + z2||X ||2

Results of Kato and Shubin⇒For any x ∈ Xk one can associate a the functionλ(z) ∈ Spec´(kz), holomorphic in a neighborhood of [0,∞) withlim<z→∞ λx (z) = 0.

Consider x λx (0) and

Pk (z) =∏

x∈Xk

(z − λx (0)).

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Page 29: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Theorem

For any k there exists a collection λkn(z) ,n ∈ N,each

holomorphic function in a neighborhood of [0,∞) so that foreach t ∈ [0,∞) the family λk

r (t), r = 1,2, · · · represent theentire family of eigenvalues of ∆X

k (t) (with their multiplicity)

Mild improvement of Witten methods shows that each rest pointx of index k provides for t very large an eigenvalue which goexponentially fast to zero. In fact much more is true

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Page 30: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

TOPOLOGY

Twisted cohomology

Is a graded vector space H∗(M; ξ) associated to(M, ξ ∈ H1(M; C).

Denote βξi := dimH i(M; ξ).

For <z large enough βzξi is constant in z.

Denote βξi := lim<z→∞ βzξi .

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Page 31: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Theorem(Novikov)If X satisfies H, MS, L with ξ a Lyapunov class for X then:

1. For <z large enough the cohomology of the cochain complexC∗(M; X , ξ)(z) and H∗(M; zξ) are naturally isomorphic.

2. One has

nk ≥ βξk∑0≤k≤r

(−1)knk ≥∑

0≤k≤r

βξk , r even

∑0≤k≤r

(−1)knk ≥∑

0≤k≤r

βξk , r odd.

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Page 32: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

Torsion

• The cochain complex C∗(M; X , ξ)(z) is equipped with a baseso it is possible to define a torsion (in case that the zξ- twistedcohomology for is trivial is a holomorphic function in z. )

• The cohomology class zξcan be interpreted as a rank1-complex representation of the fundamental group andtogether with a so called Euler structure there is a topologicalinvariant the Reidemeister torsion (in case that the zξ- twistedcohomology for is trivial is a holomorphic function in z.)

• The vector field X and some minor additional data determinean Euler structure.

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Page 33: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

It is possible to show that the sum of the log of the torsion ofC∗(M; X , ξ)(z) and of the function Z ξ(z) is exactly theReidemeister torsion of M zξ and the Euler class defined by X .This relates the functions IO,ωx ,y (z) and Z ξ(z) and the topology

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Page 34: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

• The torsion logT ∈ C associated with a cochain complex(C∗,d∗) with a nondegerate bilinear form each C i , (hence withLaplacians ∆k : Ck → Ck ,) is defined by the formula

log T = 1/2∑i≥0

(−1)i i log det ∆i

• R(g,X , ω) ∈ R is an invariant associated with a Riemannianmanifold (M,g), a vector field X with isolated rest points and aclosed one form ω defined as follows:

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Page 35: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

For an oriented Riemannian manifold M, the Riemannianmetric produces a (n − 1) differential form (the angularmomentum form)

Ψ(g) ∈ Ωn−1(TM \M)

If the vector field X has no rest points it defines the mapX : M → T (M) \M and

R(g,X , ω) :=

∫Mω ∧ X ∗(Ψ(g))

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Page 36: DYNAMICS, Geometry and TopologySpectral geometry Topology Author, Another Short Paper Title Dynamics = Smooth vector field X on a closed manifold M: Elements of Dynamics= Rest points

When the vector field X has singularities the integration is doneover M \ X and the integral might not be convergent andrequires regularization. This regularization is always possible.Geometric regularization .

Since the eigenvalues of the Laplacians ∆lai are infinitely many

the definition of det ∆lai also requires regularization. This

regularization is again possible.Zeta function regularization.

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