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Morse--Smale transversality and surjectivity of the linearized flow operator
Statement
Let be a smooth Morse function, let be a smooth Riemannian metric, and let be a full negative--gradient orbit connecting critical points . Let be the Banach space of sections for which both and tend to zero at , with the supremum norm, and let have the supremum norm. For the tangent Levi--Civita connection metric-dual to the cotangent connection, put
Then is bounded Fredholm of index , and it is surjective if and only if and are transverse at .
Facts & Assumptions
Given: The smooth , connecting orbit , and displayed and Banach spaces.
Covariant Hessians define the linearization of the gradient equation (Riemannian metrics, symmetric cotangent-bundle connections, and covariant Hessians).
The point-marked trajectory set is the stable--unstable intersection (Parametrized Morse trajectory space), using the metric-gradient version of Morse--Smale pairs.
For a continuous first-order matrix path with invertible self-adjoint limits, the operator on precisely 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).
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
Differentiating in a decaying variation gives the displayed operator by [F1]. Since converges to the critical points and is continuous, its coefficient along is bounded; hence is bounded.
By [L2], approaches and exponentially at the two ends. Parallel transport a -orthonormal frame along . In fixed endpoint coordinates its transport equation has coefficients bounded by a constant times , which are integrable on both tails; hence the frame converges at each end to an orthonormal frame. In this frame, is ordinary differentiation, so becomes , with converging to at and at . These limits are self-adjoint for the endpoint inner products and invertible because is Morse. Parallel transport preserves norms and takes to , so it identifies exactly the displayed and spaces, not a weighted Sobolev replacement.
Apply [L1] to step 2.1. Its negative-end decaying initial-value space has dimension , and its positive-end space has dimension ; therefore is Fredholm of index . By [L2], differentiating the flow along gives decaying negative-end variational solutions, and differentiating along 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 . The cokernel is consequently isomorphic, through the chosen half-line right inverses, to .
The quotient in step 3.1 vanishes exactly when the two tangent spaces span , which is transversality. By [L1], that quotient vanishes exactly when is onto. This proves the biconditional and the index assertion.
Depends on
- Morse--Smale pairs
- Parametrized Morse trajectory space
- Riemannian metrics, symmetric cotangent-bundle connections, and covariant Hessians
- A Riemannian metric has a unique Levi-Civita connection on the cotangent bundle
- Fredholm index and range of an asymptotically hyperbolic first-order operator
- Stable and unstable manifolds for a Morse gradient with an arbitrary smooth metric
Used by
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Sources
- Alberto Abbondandolo and Pietro Majer, Lectures on the Morse Complex, Lemma 3.11(ii) (standard reference, not scraped)