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Compactly supported dbar solutions on complex Euclidean space

Statement

Assume AC. Let n≥2, and let g=∑j=1ngj dzˉj be a smooth compactly supported ∂ˉ-closed (0,1)-form on Cn. Then there is a unique smooth compactly supported function u on Cn such that ∂ˉu=g. The solution vanishes on the unique unbounded connected component of Cn∖supp⁡g.

Facts & Assumptions

Given: An integer n≥2, the full Axiom of Choice, and a smooth compactly supported ∂ˉ-closed (0,1)-form g=∑j=1ngj dzˉj on Cn.

[F1]

The dzI∧dzˉJ expansion is unique, and the ∂ˉ coefficient formula differentiates each coefficient in zˉj and wedges dzˉj before its type factors (Bigraded complex forms and the Dolbeault operators).

[F2]

Under full AC, the whole-plane Cauchy transform Tkh of a compactly supported smooth function is globally smooth and satisfies ∂zˉkTkh=h (Local Cauchy transform with smooth parameters).

[F3]

For every ℓ≠k, the same whole-plane transform obeys ∂zˉℓTkh=Tk(∂zˉℓh) (Local Cauchy transform with smooth parameters).

[F4]

AC says every family of nonempty sets has a choice function (The Axiom of Choice); the Cauchy transform supplier and Cauchy–Pompeiu formula both explicitly assume AC (Local Cauchy transform with smooth parameters, The Cauchy–Pompeiu formula with fixed signs).

[F5]

The support of a differential form is the closure of its nonzero locus; the form is compactly supported when that support is compact (Compact support of a differential form).

[F8]

The complex Euclidean norm and metric agree under Cn≅R2n, and in this metric a set is compact exactly when it is closed and bounded (Complex m-space and its real coordinate dictionary).

[F9]

A set is bounded when it is empty or contained in a ball B(c,r) for some center c and radius r>0 (Bounded subset, diameter, distance from a point to a set, and distance between two sets in a metric space, Open ball, closed ball and sphere in a metric space).

[F10]

The Euclidean norm satisfies the triangle inequality ∥x+y∥≤∥x∥+∥y∥ (A norm on a real vector space, the induced metric, and the dictionary with the metric axioms).

[F11]

In Rm, the unit sphere is Sm−1 (Euclidean spheres and closed balls as subspaces of Rn) and is path-connected for m≥2 (For n≥2, the sphere Sn−1 is path-connected and connected).

[F13]

A connected component is the largest connected subset containing each of its points (Connected components, quasicomponents, and totally disconnected spaces).

[F14]

Each connected component of an open subset of Rm is open (Every connected component of an open subset of Rn is open and polygonally connected).

[F15]

For a C1 function on an open subset of Cm, the pointwise Cauchy–Riemann system implies complex differentiability, and complex differentiability at every point is holomorphy (For C1 functions, holomorphy, complex linearity of the real derivative, and the Cauchy–Riemann system agree, Holomorphic functions on an open subset of Cm). Here take m=n and match the theorem's zero-based coordinate index 0≤k<m with our one-based index j=k+1.

[F16]

A holomorphic function on a nonempty connected open set that vanishes on a nonempty open subset vanishes identically (A holomorphic function vanishing on a nonempty open subset of a domain vanishes identically).

[F17]

For a bounded domain D⊂C with C1 boundary, full AC, f∈C1(D‾), and z∈D, Cauchy–Pompeiu gives f(z)=12πi∫∂Df(ζ)ζ−z dζ+12πi∫D∂ζˉf(ζ)ζ−z dζ∧dζˉ. (The Cauchy–Pompeiu formula with fixed signs)

Proof

technique · direct
1.1F1givenalgebra

By [F1], ∂ˉg=∑a,b(∂zˉagb) dzˉa∧dzˉb; for a<b the coefficient of dzˉa∧dzˉb is ∂zˉagb−∂zˉbga. Since ∂ˉg=0 and the wedge expansion is unique, ∂zˉagb=∂zˉbga for all a,b.

1.2F8F9F10F11F12F13givenalgebra

Put K=supp⁡g. If K=∅ set R=1; otherwise [F8]–[F9] give a ball B(c,r) containing K, and [F10] lets us take R=∥c∥+r+1 so K⊂{∥z∥≤R}. Let E={∥z∥>R}. In R2n, radial segments from any two points of E to a common radius L>R, joined by a rescaled path in S2n−1 from [F11], stay in E; thus E is path-connected and connected by [F12]. It is unbounded and lies in Ω=Cn∖K. Fix e=(R+1,0,…,0)∈E and put C∞=CΩ(e). Then E⊆C∞ by [F13], and every unbounded component of Ω meets E and equals C∞ by maximality; hence this is the unique unbounded component.

1.3F1F2F4F5F6F7givenalgebra

For each j, gj≠0 implies g≠0 by [F1]; hence Kj:={z:gj(z)≠0}‾ is a closed subset of the compact set K and is compact by [F5]–[F7]. Thus gj∈Cc∞(Cn). Define u:=T1g1. Since the full AC hypothesis in [F4] is present, [F2] gives u∈C∞(Cn) and ∂zˉ1u=g1.

2.1F1F3F4F17step 1.1step 1.3givenalgebra

For j>1, [F3] and step 1.1 give ∂zˉju=T1(∂zˉjg1)=T1(∂zˉ1gj). Fix z=(z1,z2,…,zn) and choose M>max⁡(R,∣z1∣); the slice h(ζ)=gj(ζ,z2,…,zn) is C1 and vanishes on the boundary of the disc D={∣ζ∣<M} because K⊆{∥z∥≤R}. Applying [F17] to this slice at z1, its boundary term is zero. Since ∂zˉ1gj(ζ,z2,…,zn)=0 whenever ∣ζ∣>R, the area integral over D equals its whole-plane integral, namely T1(∂zˉ1gj)(z). Thus [F17] gives T1(∂zˉ1gj)(z)=gj(z). Together with step 1.3 and the scalar case of [F1], this proves ∂ˉu=g.

3.1F5F6F8F14F15F16step 1.2step 1.3step 2.1givenalgebra

The set K is closed by [F5]–[F6], so Ω is open. On Ω we have ∂ˉu=g=0; by [F15], u is holomorphic there. The open half-space V={z:Re⁡z2>R} is nonempty, connected, unbounded, and contained in Ω. For every z∈V and every integration coordinate ζ, ∥(ζ,z2,…,zn)∥≥∣z2∣≥Re⁡z2>R, so g1(ζ,z2,…,zn)=0 and the defining integral gives u(z)=0. By step 1.2, V⊆C∞; [F14] makes C∞ open. Applying [F16] on this connected open component yields u=0 throughout C∞.

4.1F5F6F8F9step 1.2step 3.1algebra

Since E⊆C∞, step 3.1 gives u=0 on the open exterior E. Therefore supp⁡u={z:u(z)≠0}‾ is closed and lies in {∥z∥≤R}⊂B(0,R+1), so it is bounded by [F9]. By [F8], this closed bounded subset of complex Euclidean space is compact, and hence u is compactly supported.

5.1F8F9F10F12F15F16step 2.1step 4.1givenalgebra∎

If v is another smooth compactly supported solution, then w=u−v is smooth and ∂ˉw=0, so [F15] makes w holomorphic on all of Cn. By [F8]–[F10], each compact support lies in a ball B(ci,ri) and the norm triangle inequality places both in one sufficiently large ball centred at 0; hence w=0 on a nonempty open exterior. Since Cn is connected by straight paths and [F12], [F16] gives w≡0. Thus u=v.

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