ConceptComplete

Pseudo-Holomorphic Curves

Pseudo-holomorphic (or JJ-holomorphic) curves, introduced by Gromov in 1985, are the primary analytical tool in modern symplectic topology. They are maps from Riemann surfaces to symplectic manifolds satisfying a Cauchy-Riemann-type equation determined by a compatible almost complex structure.


Basic Definitions

Definition7.1Almost Complex Structure

An almost complex structure on a manifold MM is a bundle endomorphism J:TMTMJ: TM \to TM with J2=idJ^2 = -\mathrm{id}. On a symplectic manifold (M,ω)(M, \omega), JJ is ω\omega-compatible if g(v,w)=ω(v,Jw)g(v,w) = \omega(v, Jw) defines a Riemannian metric (gg is symmetric and positive definite). The space J(M,ω)\mathcal{J}(M, \omega) of compatible almost complex structures is contractible.

Definition7.2$J$-Holomorphic Curve

A JJ-holomorphic curve is a smooth map u:(Σ,j)(M,J)u: (\Sigma, j) \to (M, J) from a Riemann surface (Σ,j)(\Sigma, j) satisfying the Cauchy-Riemann equation: ˉJu=12(du+Jduj)=0\bar{\partial}_J u = \frac{1}{2}(du + J \circ du \circ j) = 0. Equivalently, dudu is complex-linear: duj=Jdudu \circ j = J \circ du.

ExampleHolomorphic Spheres in $\mathbb{CP}^n$

For the standard complex structure J0J_0 on CPn\mathbb{CP}^n, J0J_0-holomorphic curves are ordinary holomorphic maps. A degree-dd rational curve u:CP1CPnu: \mathbb{CP}^1 \to \mathbb{CP}^n satisfies uωFS=dπ\int u^*\omega_{FS} = d \cdot \pi and μ(u)=2(n+1)d\mu(u) = 2(n+1)d (Maslov index in the appropriate sense).


Energy and Compactness

Definition7.3Energy of a $J$-Holomorphic Curve

The energy of a JJ-holomorphic curve u:ΣMu: \Sigma \to M is E(u)=Σuω=12Σdug2dvolΣE(u) = \int_\Sigma u^*\omega = \frac{1}{2}\int_\Sigma |du|_g^2 \, \mathrm{dvol}_\Sigma. The equality of topological and analytic energy is a consequence of the Cauchy-Riemann equation and is the key to compactness.

RemarkGromov Compactness

The Gromov compactness theorem states that a sequence of JJ-holomorphic curves with bounded energy has a subsequence converging to a stable map (a nodal curve with holomorphic components). Energy can concentrate at points, creating "bubbles" — sphere components attached at nodes. This compactness is essential for defining Gromov-Witten invariants.