ConceptComplete

Floer Homology

Floer homology is an infinite-dimensional Morse theory for the action functional on the loop space of a symplectic manifold. It provides the primary tool for proving the Arnold conjecture and has become one of the most powerful invariants in symplectic topology.


Construction

Definition8.1Floer Chain Complex

For a non-degenerate Hamiltonian H:S1×M→RH: S^1 \times M \to \mathbb{R} on a compact symplectic manifold (M,ω)(M, \omega), the Floer chain complex CF∗(M,H)CF_*(M, H) is the Z2\mathbb{Z}_2-vector space generated by 1-periodic orbits of XHX_H. The differential counts Floer trajectories: solutions u:R×S1→Mu: \mathbb{R} \times S^1 \to M of the Floer equation ∂su+Jt(∂tu−XH(t,u))=0\partial_s u + J_t(\partial_t u - X_H(t, u)) = 0 converging to periodic orbits as s→±∞s \to \pm\infty.

Definition8.2Floer Homology

The Hamiltonian Floer homology HF∗(M,ω)HF_*(M, \omega) is the homology H∗(CF∗,∂)H_*(CF_*, \partial). The key properties: ∂2=0\partial^2 = 0 (from Gromov compactness for 1-dimensional moduli spaces), and HF∗HF_* is independent of HH and JJ (invariance via continuation maps). For a compact symplectic manifold, HF∗(M)≅H∗(M;Z2)HF_*(M) \cong H_*(M; \mathbb{Z}_2) (or QH∗(M)QH_*(M) over the Novikov ring).

ExampleFloer Homology of $T^{2n}$

For the torus T2nT^{2n} with standard symplectic form, HF∗(T2n)≅H∗(T2n;Z2)HF_*(T^{2n}) \cong H_*(T^{2n}; \mathbb{Z}_2) has total dimension 22n2^{2n}. Since dim⁡CF∗≥dim⁡HF∗\dim CF_* \geq \dim HF_*, every non-degenerate Hamiltonian on T2nT^{2n} has at least 22n2^{2n} periodic orbits, proving the Arnold conjecture.


Grading and Ring Structure

RemarkConley-Zehnder Index

When c1(TM)=0c_1(TM) = 0 or c1(TM)∣π2=0c_1(TM)|_{\pi_2} = 0, the Floer complex admits a Z\mathbb{Z}-grading by the Conley-Zehnder index, which measures the winding of the linearized flow along a periodic orbit relative to a trivialization. The differential decreases the grading by 1.

Definition8.3Pair-of-Pants Product

The pair-of-pants product HF∗(H1)⊗HF∗(H2)→HF∗(H1#H2)HF_*(H_1) \otimes HF_*(H_2) \to HF_*(H_1 \# H_2) is defined by counting holomorphic maps from a pair-of-pants surface (sphere minus three discs) with Lagrangian/periodic boundary conditions. This gives HF∗HF_* the structure of a ring isomorphic to the quantum cohomology ring QH∗(M)QH^*(M).