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TheoremStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-6-luna)verified 2026-10-22 (gpt-6.1-sol)
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Picard range and pseudoinverse-domain criterion

Statement

Assume the Axiom of Countable Choice. Let K:X→Y be a compact linear map between real or complex Hilbert spaces, with Hilbert adjoint K∗:Y→X. Write N>0:={1,2,3,…}. If R(K) has finite dimension r∈N, put J={1,…,r}, interpreted as empty when r=0; if R(K) is infinite-dimensional, put J=N>0. Thus J indexes exactly the positive singular values sj>0 in nonincreasing order. Let (vj)j∈J and (uj)j∈J be complete orthonormal families in N(K)⊥ and R(K)‾, respectively, with Kvj=sjuj and K∗uj=sjvj. The empty sum is zero, finite J uses a finite sum, and infinite J uses the norm-convergent series whenever the stated square-summability condition holds. Use inner products linear in the first argument. Define the Picard sum PK(y):=∑j∈J∣⟨y,uj⟩Y∣2sj2,y∈Y. Then:

  1. The exact equation Kx=y is solvable if and only if y⊥N(K∗) and PK(y)<∞.

  2. The domain of the Hilbert-space Moore–Penrose inverse is D(K†)=R(K)⊕R(K)⊥={y∈Y:PK(y)<∞}, and for every y∈D(K†), K†y=∑j∈J⟨y,uj⟩Ysjvj. Thus the orthogonal component in R(K)⊥=N(K∗) is discarded by K†; exact range membership additionally requires that component to be zero.

Singular-system diagram

For a fixed positive singular index j, the diagram records the domain/codomain action on its one-dimensional singular directions:

FFXY¸7!sj¸¸7!¸vj¸7!¸ujK

The two composites agree because K(λvj)=λKvj=λsjuj. This diagram explains the singular-pair convention; no proof step relies on it.

Facts & Assumptions

Given: Countable Choice, the compact Hilbert-space model K:X→Y, its adjoint K∗, and the positive singular system described in the statement.

[F1]

The model supplies real or complex Hilbert parameter/data spaces and a compact linear forward map (Compact linear inverse model between Hilbert spaces).

[F2]

The compact SVD supplies the positive singular values, complete orthonormal right and left singular families, the singular relations, and the operator expansion (Singular value decomposition for compact operators).

[F3]

(R(K))⊥=N(K∗) and R(K)‾=(N(K∗))⊥ (Kernel–range orthogonality for Hilbert adjoints).

[F4]

⟨Kx,y⟩Y=⟨x,K∗y⟩X (The Hilbert-space adjoint of a bounded operator).

[F5]

Finite Bessel inequality: ∑j∈F∣⟨x,ej⟩∣2≤∥x∥2 for every finite orthonormal family (The finite Bessel inequality and best approximation by a finite orthonormal family).

[F6]

Finite orthogonal sums satisfy Pythagoras (Pythagoras and finite orthogonal sums).

[F7]

On a complete orthonormal family, the finite Fourier sums converge in norm to each vector in its closed span (Fourier expansion in a Hilbert space).

[F8]

Every closed subspace of a Hilbert space has an orthogonal decomposition (Orthogonal decomposition by a closed subspace).

[F9]

Hilbert spaces are complete and Cauchy–Schwarz makes the inner product continuous in either argument (Hilbert space, Cauchy–Schwarz: ∣⟨x,y⟩∣≤∥x∥ ∥y∥, with equality exactly for dependent pairs).

[F10]

For r+z with r∈R(K) and z∈R(K)⊥, the inverse returns the minimum-norm preimage of r and annihilates z (Hilbert-space Moore–Penrose inverse).

[F11]

A compact linear operator is bounded and hence continuous in norm (Compact linear operator).

[A1]

Countable Choice is the hypothesis in the compact SVD and Hilbert Fourier expansion used here (The Axiom of Countable Choice (ACω)).

Proof

technique · direct
1.1givenF2F3F4F5A1algebra

Suppose y=Kx. Then y⊥N(K∗) by [F3]. For each j∈J, the adjoint identity and singular relation give ⟨y,uj⟩Y=⟨Kx,uj⟩Y=⟨x,K∗uj⟩X=sj⟨x,vj⟩X. Applying [F5] to finite subsets of the orthonormal family (vj) shows PK(y)=∑j∈J∣⟨x,vj⟩X∣2≤∥x∥X2<∞. This proves necessity in claim 1.

1.2F2F3F6F9A1constructalgebra

Now let y⊥N(K∗) and PK(y)<∞. By [F3], y∈R(K)‾. For finite J take the finite sum; for infinite J let xN=∑j=1Nsj−1⟨y,uj⟩Yvj. For M>N, [F6] gives ∥xM−xN∥X2=∑j=N+1Msj−2∣⟨y,uj⟩Y∣2, whose tails tend to zero because PK(y)<∞. Thus (xN) is Cauchy and converges to x∈X by [F9]. The complete right singular family places x in N(K)⊥.

2.1step 1.2F1F2F7F10F11A1algebra

By [F11], applying K to the finite sums and passing to the limit gives Kx=lim⁡N→∞KxN=lim⁡N→∞∑j=1N⟨y,uj⟩Yuj=y, where the last equality is [F7] on R(K)‾. The finite-J case is the same equality with a finite sum. Since x∈N(K)⊥ and Kx=y, [F10] identifies x=K†y. This proves sufficiency in claim 1 and the formula there.

3.1step 1.2step 2.1F3F7F8F10A1construct

For arbitrary y∈Y, apply [F8] to the closed subspace M=R(K)‾ and write y=p+q with p∈M and q∈M⊥. Since R(K)⊆M, q∈R(K)⊥. The Fourier coefficients of p are ⟨p,uj⟩Y=⟨y,uj⟩Y, and [F7] expands p in the complete left singular family. If PK(y)<∞, the construction in steps 1.2–2.1 applied to p∈M=(N(K∗))⊥ gives p∈R(K) and K†p=∑jsj−1⟨y,uj⟩Yvj; hence y=p+q∈R(K)⊕R(K)⊥=D(K†) and [F10] gives the displayed formula.

4.1step 1.1F3F10∎

Conversely, let y=r+q∈D(K†) with r∈R(K) and q∈R(K)⊥. By [F3], q∈N(K∗) and each uj∈N(K∗)⊥, so ⟨q,uj⟩Y=0. Step 1.1 applied to r shows PK(y)=PK(r)<∞; [F10] gives K†y=K†r and the same series formula. Thus the domain is exactly the set where the Picard sum is finite, completing claim 2.

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Dependency tree · two levels

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