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Dolbeault green operator is compact on the orthogonal complement of the kernel

Statement

Assume the Axiom of Choice (The Axiom of Choice). It enters through the Sobolev localization and local compactness interfaces, and it supplies Dependent Choice for the sequential compact-operator criterion; the Lax–Milgram and compact self-adjoint norm-attainment arguments use only Countable Choice (The Axiom of Countable Choice (ACω), AC implies DC implies countable choice). Let X be a compact Riemann surface, let E→X be a holomorphic line bundle with Hermitian metric h, and let g be a compatible Riemannian metric. Use the Hilbert spaces, maximal Dolbeault operator Dˉ, Hilbert adjoint Dˉ∗, and nonnegative self-adjoint Dolbeault Laplacian Δ′′ of The maximal Dolbeault operator and its Hilbert adjoint on a compact Riemann surface. Write H:=ker⁡Δ′′ and H⊥ for its orthogonal complement in L2:=L02⊕L12. For u=u0+u1 set V:=dom⁡Dˉ⊕dom⁡Dˉ∗,∥u∥V2:=∥u∥L22+∥Dˉu0∥L22+∥Dˉ∗u1∥L22. By Gårding estimates for the Dolbeault Laplacian on a compact Riemann surface, V=H1(X,Λ0,∙T∗X⊗E) with equivalent norms. Give V the first-variable-linear form inner product a(u,v):=⟨u,v⟩L2+⟨Dˉu0,Dˉv0⟩L2+⟨Dˉ∗u1,Dˉ∗v1⟩L2.

  1. Boundary operator. There is a unique bounded linear operator B:L2→V (A bounded linear operator between normed spaces) satisfying a(Bf,v)=⟨f,v⟩L2(f∈L2, v∈V). It obeys ∥Bf∥V≤∥f∥L2 and ∥Bf∥H2≤C∥f∥L2, lies in dom⁡Δ′′, and satisfies (I+Δ′′)Bf=f. As an operator on L2, B is injective, self-adjoint and positive; B∣H=I, ker⁡(I−B)=H, and B(H⊥)⊆H⊥.

  2. Compactness. The operator B:L2→L2 is compact.

  3. Green operator. The restriction of I−B to H⊥ is boundedly invertible. The operator G:=B(I−B)−1:H⊥⟶H⊥ is compact, self-adjoint and positive, has trivial kernel, and obeys ran⁡G=dom⁡Δ′′∩H⊥,ran⁡G‾=H⊥. It satisfies the Green identities Δ′′Gf=f(f∈H⊥),GΔ′′u=u(u∈dom⁡Δ′′∩H⊥), and maps H⊥ boundedly into H2.

Facts & Assumptions

Given: The compact Riemann surface, the supplied Hermitian and Riemannian metrics, the operators and spaces in the Statement, and full AC.

[F1]

The pointwise Hermitian L2 pairing is first-variable-linear, its completion is a complex Hilbert space, and smooth forms are dense; Hilbert space means a complete inner-product space (Hermitian metric and L2 pairing on a compact Riemann surface, Hilbert space).

[F2]

The maximal operator and its adjoint are densely defined and closed, Δ′′ is self-adjoint and nonnegative with the block-composition domain, and for u∈dom⁡Δ′′, ⟨Δ′′u,u⟩=∥Dˉu0∥L22+∥Dˉ∗u1∥L22 (The maximal Dolbeault operator and its Hilbert adjoint on a compact Riemann surface).

[F3]

The first-order estimate identifies V with H1, proves smooth graph-norm density, and identifies the form equation against smooth tests with the distributional equation for Δ′′. A distributional solution u∈H1 of Δ′′u=f∈L2 lies in H2 and obeys ∥u∥H2≤C0(∥f∥L2+∥u∥L2) (Gårding estimates for the Dolbeault Laplacian on a compact Riemann surface).

[F4]

The local formulas for Dˉ and Dˉ∗ have smooth coefficients. If u∈H2, then their local coefficients applied to u lie in H1: weak derivatives of an H2 coefficient are H1, and multiplication by a smooth coefficient preserves H1 by the distributional Leibniz rule. Consequently Dˉu0∈dom⁡Dˉ∗ and Dˉ∗u1∈dom⁡Dˉ, so u∈dom⁡Δ′′ (The Dolbeault adjoint and Laplacian: local formulas and ellipticity, Leibniz rule for distributions).

[F5]

On a Hilbert space, a bounded coercive sesquilinear form and a bounded conjugate-linear functional have a unique Lax–Milgram solution; if the coercivity constant is 1, its form norm is at most the functional norm. A linear map is bounded when a constant controls its output norm by its input norm. Cauchy–Schwarz bounds the form and functional, and Lax–Milgram uses Countable Choice (Bounded, coercive and symmetric sesquilinear forms, The Lax--Milgram theorem, The Axiom of Countable Choice (ACω), A bounded linear operator between normed spaces, Cauchy–Schwarz: ∣⟨u,v⟩∣≤∥u∥∥v∥, with equality exactly for linearly dependent vectors).

[F6]

A sequence bounded in Wloc1,2 on a Euclidean open set has a subsequence converging in Lloc2 under AC (Local Lp compactness of Wloc1,p-bounded sequences).

[F7]

A bounded linear operator is compact when every bounded sequence has an image subsequence converging in norm; the sequential characterization assumes DC, and AC implies DC (Compact linear operator, Sequential characterization of compact operators, AC implies DC implies countable choice).

[F8]

For a nonzero compact self-adjoint operator T on a Hilbert space, one of ∥T∥ and −∥T∥ is an eigenvalue; self-adjointness and positivity have their bounded-operator meanings, and ∥T∥ is the operator norm. This fact assumes Countable Choice (Norm point of a compact self adjoint operator is an eigenvalue up to sign, Self-adjoint, positive, unitary and normal operators, The operator norm as the least bound and as the unit-sphere or unit-ball supremum, The Axiom of Countable Choice (ACω)).

[F9]

If T is bounded with ∥T∥<1 on a Banach space, I−T has inverse ∑n≥0Tn with norm at most (1−∥T∥)−1 (Neumann series and small perturbations of bounded inverses).

[F10]

An orthogonal complement is the subspace of vectors orthogonal to the given set and is closed (Orthogonality and the orthogonal complement, Orthogonal complements are closed).

[F12]

Full AC supplies the Countable Choice instances used by Lax–Milgram and norm attainment (The Axiom of Choice, The Axiom of Countable Choice (ACω)).

[F13]

For a linear subspace of a Hilbert space, its double orthogonal complement is its closure (The double orthogonal complement of a subspace is its closure).

Proof

technique · Solve the positive form equation by Lax–Milgram, use the local Rellich theorem to prove compactness, then invert $I-B$ on the orthogonal complement of the harmonic kernel
1.1F1F3F5F12algebra

The form a is Hermitian and bounded by ∥u∥V∥v∥V, and a(u,u)=∥u∥V2, so it is coercive with constant 1. For each f∈L2, v↦⟨f,v⟩L2 is conjugate-linear and has norm at most ∥f∥L2 on V. Since V is Hilbert by [F3], Lax–Milgram [F5] gives a unique Bf∈V with a(Bf,v)=⟨f,v⟩ for every v∈V, and ∥Bf∥V≤∥f∥L2. Uniqueness makes f↦Bf linear, and this estimate makes it bounded into both V and L2.

1.2F2F3F4algebra

For every smooth test form v, the defining equation of Bf gives ⟨Dˉ(Bf)0,Dˉv0⟩+⟨Dˉ∗(Bf)1,Dˉ∗v1⟩=⟨f−Bf,v⟩. By [F3] this is the distributional equation Δ′′Bf=f−Bf; the H2 estimate in [F3] applies because Bf∈V=H1 and f−Bf∈L2, yielding ∥Bf∥H2≤C0(∥f−Bf∥+∥Bf∥)≤3C0∥f∥. Fact [F4] now puts Bf in dom⁡Δ′′, so the distributional identity is the operator identity (I+Δ′′)Bf=f. Conversely, for u∈dom⁡Δ′′, set f=(I+Δ′′)u. Then z=Bf−u lies in dom⁡Δ′′ and (I+Δ′′)z=0; taking its pairing with z and using [F2] gives 0=∥z∥2+∥Dˉz0∥2+∥Dˉ∗z1∥2, so z=0 and B(I+Δ′′)u=u.

1.3F1algebra

The equation with v=Bg gives a(Bf,Bg)=⟨f,Bg⟩; Hermitian symmetry of a then gives ⟨Bf,g⟩=⟨f,Bg⟩, so B is self-adjoint. Taking g=f shows ⟨Bf,f⟩=a(Bf,Bf)≥0, so B is positive. If Bf=0, its defining equation gives ⟨f,v⟩=0 for every v∈V; smooth forms are dense in L2 by [F1], hence f=0 and B is injective. Also ∥Bf∥L2≤∥Bf∥V≤∥f∥L2, so ∥B∥≤1.

2.1F1F2F10step 1.3algebra

If h∈H, the energy identity [F2] gives Dˉh0=0 and Dˉ∗h1=0, whence h∈V and a(h,v)=⟨h,v⟩ for all v∈V; uniqueness gives Bh=h. Conversely, if Bx=x, then x∈V and testing its defining equation with v=x gives ∥x∥V2=∥x∥L22, so both first-order terms vanish. The block domain in [F2] then gives x∈dom⁡Δ′′ and Δ′′x=0. Thus ker⁡(I−B)=H. Self-adjointness and B∣H=I imply B(H⊥)⊆H⊥.

2.2F3F6F7F12step 1.2algebra

Let (fn) be bounded in L2 and put un=Bfn. Step 1.2 bounds (un) in the fixed finite-chart H2 norm, so every partitioned local coefficient is bounded in Wloc1,2; [F6] gives a subsequence converging in Lloc2 for each chart coefficient. Successively taking subsequences over the finitely many charts and degrees gives one subsequence converging in L2 on every compact support of the fixed partition; summing these finitely many weighted coefficient norms gives convergence in global L2. Thus B takes every bounded sequence to a sequence with a norm-convergent subsequence. By [F7] and [F12], the sequential characterization proves that B:L2→L2 is compact.

3.1F1F7F8F9F10F11F12step 1.3step 2.1step 2.2algebra

The closed subspace H⊥ is invariant under B by step 2.1. For any bounded sequence in H⊥, compactness of B from step 2.2 gives a subsequence whose images converge in L2; its limit remains in H⊥ by [F10], so [F7] shows that T:=B∣H⊥ is compact on H⊥. This closed subspace is Hilbert by [F1, F11]. It is self-adjoint, positive and has norm at most 1 by step 1.3. If T=0, its norm is already less than 1; this includes H⊥={0}. Otherwise [F8] gives an eigenvalue equal to ∥T∥ or −∥T∥; positivity excludes the negative value, and if ∥T∥=1 its unit eigenvector would lie in ker⁡(I−B)∩H⊥={0} by step 2.1, a contradiction. Hence r:=∥T∥<1, and [F9] gives the bounded inverse C:=(I−T)−1=∑n≥0Tn on H⊥, with ∥C∥≤(1−r)−1.

4.1F1F7F9step 1.3step 2.1step 3.1algebra

The series G:=TC=∑n≥1Tn converges in operator norm by [F9]. Each power Tn is self-adjoint and positive: for n=2m, ⟨Tnx,x⟩=∥Tmx∥2, and for n=2m+1, it equals ⟨T(Tmx),Tmx⟩≥0. Therefore G is self-adjoint and positive. For any bounded sequence (xn) in H⊥, boundedness of C makes (Cxn) bounded; compactness of T from step 3.1 gives a subsequence for which Gxn=TCxn converges, so [F7] proves compactness of G. It is injective because both T and C are injective. For f∈H⊥, put y=Cf; step 1.2 gives Gf=By∈dom⁡Δ′′∩H⊥ and Δ′′Gf=(I−B)y=f.

5.1F1F2F9F10F13step 1.2step 4.1algebra∎

If u∈dom⁡Δ′′∩H⊥, self-adjointness of Δ′′ and Δ′′h=0 for h∈H imply Δ′′u∈H⊥. Both u and GΔ′′u lie in dom⁡Δ′′ and have the same Laplacian by step 4.1, so their difference belongs to H∩H⊥={0}. Thus GΔ′′u=u and ran⁡G=dom⁡Δ′′∩H⊥. If z⊥ran⁡G, self-adjointness gives ⟨x,Gz⟩=0 for all x∈H⊥, hence Gz=0 and z=0; [F13] now gives ran⁡G‾=H⊥. Finally, ∥Gf∥H2=∥B(Cf)∥H2≤3C0∥C∥∥f∥L2 by step 1.2 and [F9].

Source notes

Demailly's Ch. VI §2 (2.2) states the compact Rellich inclusion on a compact manifold. The bundle-valued compactness step is assembled chartwise from the library's local compactness theorem. The construction of B, the norm gap on H⊥, and the corrected Green range are established here from the exact operator-theoretic suppliers. Demailly's separate Ch. VI §3.3 Hodge statements assume a flat Hermitian connection and are not used for this result.

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