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Morse--Smale transversality and surjectivity of the linearized flow operator

Statement

Let f be a smooth Morse function, let g be a smooth Riemannian metric, and let γ be a full negative-g-gradient orbit connecting critical points p,q. Let Eγ=C01(R,γ∗TM) be the Banach space of C1 sections for which both ξ and ∇tξ tend to zero at ±∞, with the supremum C1 norm, and let Fγ=C00(R,γ∗TM) have the supremum norm. For the tangent Levi--Civita connection metric-dual to the cotangent connection, put

Dγξ=∇tξ+∇ξgrad⁡gf.

Then Dγ:Eγ→Fγ is bounded Fredholm of index λ(p)−λ(q), and it is surjective if and only if Wu(p) and Ws(q) are transverse at γ(0).

Facts & Assumptions

Given: The smooth f,g, connecting orbit γ, and displayed C01 and C00 Banach spaces.

[F1]

Covariant Hessians define the linearization of the gradient equation (Riemannian metrics, symmetric cotangent-bundle connections, and covariant Hessians).

[F2]

The point-marked trajectory set is the stable--unstable intersection (Parametrized Morse trajectory space), using the metric-gradient version of Morse--Smale pairs.

[L1]

For a continuous first-order matrix path with invertible self-adjoint limits, the operator on precisely C01(R)→C00(R) is Fredholm; its index and range are determined by the two decaying initial-value spaces (Fredholm index and range of an asymptotically hyperbolic first-order operator).

[L2]

The stable and unstable manifolds for an actual smooth metric gradient have the expected dimensions, and tangent variations along a converging orbit decay exponentially at the appropriate end (Stable and unstable manifolds for a Morse gradient with an arbitrary smooth metric).

Proof

technique · direct
1.1F1given

Differentiating γ˙+grad⁡gf(γ)=0 in a decaying variation gives the displayed operator by [F1]. Since γ converges to the critical points and ∇grad⁡gf is continuous, its coefficient along γ is bounded; hence Dγ:Eγ→Fγ is bounded.

2.1F1L2step 1.1algebra

By [L2], γ(t) approaches p and q exponentially at the two ends. Parallel transport a g-orthonormal frame along γ. In fixed endpoint coordinates its transport equation has coefficients bounded by a constant times ∣γ˙(t)∣, which are integrable on both tails; hence the frame converges at each end to an orthonormal frame. In this frame, ∇t is ordinary differentiation, so Dγ becomes z′−A(t)z, with A(t) converging to −gp−1Hess⁡pf at −∞ and −gq−1Hess⁡qf at +∞. These limits are self-adjoint for the endpoint inner products and invertible because f is Morse. Parallel transport preserves norms and takes ∇tξ to z′, so it identifies exactly the displayed C01 and C00 spaces, not a weighted Sobolev replacement.

3.1L1L2step 2.1algebra

Apply [L1] to step 2.1. Its negative-end decaying initial-value space has dimension λ(p), and its positive-end space has dimension dim⁡M−λ(q); therefore Dγ is Fredholm of index λ(p)−λ(q). By [L2], differentiating the flow along Wu(p) gives decaying negative-end variational solutions, and differentiating along Ws(q) gives decaying positive-end ones. Both tangent spaces have exactly the corresponding dimensions, so inclusion implies equality with the two ODE initial-value spaces at γ(0). The cokernel is consequently isomorphic, through the chosen half-line right inverses, to Tγ(0)M/(Tγ(0)Wu(p)+Tγ(0)Ws(q)).

4.1F2L1step 3.1algebra∎

The quotient in step 3.1 vanishes exactly when the two tangent spaces span Tγ(0)M, which is transversality. By [L1], that quotient vanishes exactly when Dγ is onto. This proves the biconditional and the index assertion.

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