[Paper Review] Morse homology on noncompact manifolds
This paper establishes the relationship between three variants of Morse homology on noncompact manifolds: Novikov-type homology $HM$, the direct-involution limit $ar{HM}$, and the inverse-direct limit $\underline{HM}$, under field coefficients. It proves that $ar{HM} \cong HM$ via an isomorphism, while the canonical map $\kappa: \bar{HM} \to \underline{HM}$ is surjective but not necessarily injective, resolving a key question in Floer theory and clarifying the algebraic structure of Morse homology in noncompact settings.
Given a Morse function on a manifold whose moduli spaces of gradient flow lines for each action window are compact up to breaking one gets a bidirect system of chain complexes. There are different possibilities to take limits of such a bidirect system. We discuss in this note the relation between these different limits.
Motivation & Objective
- To clarify the algebraic relationship between three distinct limits of Morse homology on noncompact manifolds: $HM$, $\bar{HM}$, and $\underline{HM}$.
- To determine under what conditions the canonical maps between these homology groups are isomorphisms, surjections, or injections.
- To resolve a question raised by K. Ono regarding whether the map $\bar{\rho}: HM \to \bar{HM}$ is an isomorphism in the context of Floer homology.
- To provide an algebraic explanation for why $HM \cong \bar{HM}$ in cases like weakly monotone symplectic manifolds, where direct computation previously showed equality.
- To demonstrate via counterexample that $\kappa: \bar{HM} \to \underline{HM}$ need not be injective, even when $\bar{HM} \neq 0$.
Proposed method
- The authors define Morse homology $HM^{[a,b]}_*$ for fixed action windows $[a,b]$, assuming compactness of moduli spaces of gradient flow lines up to breaking.
- They construct a bidirect system of chain complexes indexed by action windows $[a,b]$, enabling the formation of inverse and direct limits.
- They define three homology groups: $HM$ via Novikov completion of the chain complex, $\bar{HM} = \varinjlim_{b \to \infty} \varprojlim_{a \to -\infty} HM^b_a$, and $\underline{HM} = \varprojlim_{a \to -\infty} \varinjlim_{b \to \infty} HM^b_a$.
- They analyze the canonical maps $\kappa: \bar{HM} \to \underline{HM}$, $\bar{\rho}: HM \to \bar{HM}$, and $\underline{\rho}: HM \to \underline{HM}$, proving their properties under field coefficients.
- They use an explicit counterexample with a disjoint union of lines $\bigsqcup_{n=1}^\infty \mathbb{R}$ to show $\kappa$ is not injective, while $\bar{HM} \neq 0$.
- They prove $\bar{\rho}$ is an isomorphism and $\kappa$ is surjective by analyzing the structure of homology classes and using divisibility arguments in $\mathbb{Z}$-modules.
Experimental results
Research questions
- RQ1Is the canonical map $\bar{\rho}: HM \to \bar{HM}$ an isomorphism when coefficients are a field?
- RQ2What is the relationship between $\bar{HM}$ and $\underline{HM}$, and is the map $\kappa: \bar{HM} \to \underline{HM}$ injective?
- RQ3Does the isomorphism $HM \cong \bar{HM}$ hold in general for noncompact manifolds with field coefficients?
- RQ4Can the algebraic structure of Morse homology on noncompact manifolds be axiomatized to extend beyond finite-dimensional settings?
- RQ5Why does $\kappa$ fail to be injective in general, and what structural features of the system cause this?
Key findings
- The map $\bar{\rho}: HM \to \bar{HM}$ is an isomorphism when homology is computed with field coefficients, establishing that the Novikov completion and the direct-involution limit agree.
- The map $\kappa: \bar{HM} \to \underline{HM}$ is surjective but not necessarily injective, as shown by a counterexample with $\underline{HM} = 0$ and $\bar{HM} \neq 0$.
- The counterexample involves a disjoint union of lines $\bigsqcup_{n=1}^\infty \mathbb{R}$ with Morse functions having critical points at $f(\overline{c}_n) = n$ and $f(\underline{c}_n) = -n$, leading to nontrivial $\bar{HM}$ but trivial $\underline{HM}$.
- The non-injectivity of $\kappa$ arises from the failure of Mittag-Leffler condition in the inverse limit system, particularly due to unbounded growth in transition maps.
- The proof that $\bar{HM} = 0$ in the counterexample relies on divisibility by arbitrarily high powers of 2 in the transition maps, forcing coefficients to vanish.
- The existence of a nontrivial class $\xi = \sum a_j \underline{c}_j$ in $HM$ with $a_j \in \{0,1\}$, not in the image of $\partial$, shows $HM \neq 0$, while $\bar{HM} = 0$, confirming the counterexample.
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This review was created by AI and reviewed by human editors.