ProofComplete

Proof that 2=0\partial^2 = 0 in Floer Homology

The fundamental property of the Floer differential is 2=0\partial^2 = 0, which ensures the Floer chain complex is indeed a chain complex. The proof relies on the compactification of 1-dimensional moduli spaces of Floer trajectories.


Setup

Theorem8.3$\\partial^2 = 0$

In the Floer chain complex CF(H,J)CF_*(H, J), the differential :CFkCFk1\partial: CF_k \to CF_{k-1} defined by x=μ(y)=k1n(x,y)y\partial x = \sum_{\mu(y) = k-1} n(x, y) \cdot y (where n(x,y)Z2n(x, y) \in \mathbb{Z}_2 counts rigid Floer trajectories from xx to yy) satisfies 2=0\partial^2 = 0.


Proof

Proof

We need to show that for generators xx (index kk) and zz (index k2k - 2): 2x,z=μ(y)=k1n(x,y)n(y,z)=0(mod2).\langle \partial^2 x, z \rangle = \sum_{\mu(y) = k-1} n(x, y) \cdot n(y, z) = 0 \pmod{2}.

Consider the moduli space M(x,z)\mathcal{M}(x, z) of Floer trajectories from xx to zz. Since μ(x)μ(z)=2\mu(x) - \mu(z) = 2, this moduli space has virtual dimension 1 (after quotienting by the R\mathbb{R}-translation).

Compactification: By Gromov compactness, M(x,z)\overline{\mathcal{M}}(x, z) is a compact 1-manifold with boundary. Boundary points correspond to broken trajectories: pairs (u1,u2)(u_1, u_2) where u1M(x,y)u_1 \in \mathcal{M}(x, y) and u2M(y,z)u_2 \in \mathcal{M}(y, z) for some intermediate orbit yy with μ(y)=k1\mu(y) = k - 1.

Boundary structure: The boundary of the compact 1-manifold M(x,z)\overline{\mathcal{M}}(x, z) is: M(x,z)=μ(y)=k1M(x,y)×M(y,z).\partial \overline{\mathcal{M}}(x, z) = \bigsqcup_{\mu(y) = k-1} \mathcal{M}(x, y) \times \mathcal{M}(y, z).

Counting: Since a compact 1-manifold with boundary has an even number of boundary points: yn(x,y)n(y,z)0(mod2).\sum_y n(x, y) \cdot n(y, z) \equiv 0 \pmod{2}.

This holds for all x,zx, z, proving 2=0\partial^2 = 0. \square

RemarkAnalytical Foundations

The proof requires: (1) transversality: the moduli spaces M(x,y)\mathcal{M}(x,y) are smooth manifolds of the expected dimension for generic JJ; (2) compactness: sequences in M(x,z)\mathcal{M}(x,z) converge to broken trajectories (no energy loss to sphere bubbles when [ω]π2=0[\omega]|_{\pi_2} = 0, or more generally controlled by the Novikov ring); (3) gluing: broken trajectories can be "glued" back to nearby unbroken ones, ensuring the boundary identification is correct.

ExampleFinite-Dimensional Analogy

In ordinary Morse theory, 2=0\partial^2 = 0 follows from the same argument: the 1-dimensional moduli space of gradient flow lines between critical points of index difference 2 is a compact 1-manifold whose boundary counts broken flow lines. Floer homology is the infinite-dimensional generalization of this picture.