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Tame J-holomorphic area equals metric Dirichlet energy

Statement

Let (M,ω,J) be the tame almost-complex data of Symplectic and almost-complex curve data, and let (Σ,j) be a Riemann surface. A smooth Riemannian metric h on Σ is j-compatible when h(jξ,jη)=h(ξ,η) for all tangent vectors ξ,η. Assume that h is j-compatible. Set gJsym(v,w)=12(ω(v,Jw)+ω(w,Jv)), which is positive definite because J is tame. At z∈Σ, define the Hilbert--Schmidt norm of duz:(TzΣ,hz)→(Tu(z)M,gJsym) by ∣duz∣gJsym,h2=∑a=12gJsym(duz(ea),duz(ea)), where (e1,e2) is any hz-orthonormal basis; this sum is independent of that basis. Let dvol⁡h be the area measure induced by h. If u:Σ→M is a smooth J-holomorphic map with finite symplectic area Eω(u), then its Dirichlet energy ED(u)=12∫Σ∣du∣gJsym,h2 dvol⁡h equals the symplectic area Eω(u)=∫Σu∗ω, and both are nonnegative. If J is compatible, gJsym(v,w)=ω(v,Jw). For tame but noncompatible J, the symmetrized form is the metric; the unsymmetrized form ω(⋅,J⋅) is not assumed symmetric.

Facts & Assumptions

Given: The symplectic form, tame almost-complex structure, domain, map, and metrics in the statement.

[F1]

Symplectic and almost-complex curve data: J2=−I, du∘j=J∘du, tameness means ω(v,Jv)>0 for v≠0, and gJsym(v,w)=12(ω(v,Jw)+ω(w,Jv)); ω is a skew-symmetric two-form.

Proof

1.1givenF1algebra

At any point, gJsym is smooth and symmetric by its definition, and gJsym(v,v)=ω(v,Jv)>0 for every nonzero v by tameness. Thus it is a Riemannian metric. Choose a unit vector e at the point. Since h is j-compatible, h(je,je)=h(e,e)=1 and h(e,je)=h(je,j2e)=−h(je,e), so h(e,je)=0. Thus (e,je) is a positively oriented h-orthonormal basis of TΣ. Put v=du(e). The Cauchy–Riemann equation gives du(je)=Jv. Using J2=−I and skew-symmetry of ω gives gJsym(v,Jv)=0 and gJsym(Jv,Jv)=gJsym(v,v)=ω(v,Jv).

2.1givenF1step 1.1algebra

The area density in this basis is (u∗ω)(e,je)=ω(v,Jv), while the Dirichlet density is 12(∣du(e)∣2+∣du(je)∣2)=gJsym(v,v). Thus the densities agree pointwise, including at points where du=0; integrating gives ED(u)=Eω(u). Tameness makes this common density nonnegative, and the finite-area hypothesis makes both integrals finite.

3.1F1step 1.1∎

If J is compatible, ω(⋅,J⋅) is symmetric by definition, so its symmetrization is itself. For a merely tame J, only gJsym is used as the metric; no Riemannian metric is inferred from the unsymmetrized form.

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