Alphabeta Math
TheoremStatement: AI-adaptedProof: AI-adaptedPipeline-generatedaudited 2026-09-22
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Fredholm index is locally constant

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let X and Y be Banach spaces over the same scalar field. Then the Fredholm operators X→Y (Fredholm operator cokernel and index) form an open subset of the space B(X,Y) of bounded linear operators with the operator norm (A bounded linear operator between normed spaces, The operator norm as the least bound and as the unit-sphere or unit-ball supremum): for every Fredholm T there is a real δ>0 such that every bounded A:X→Y with ∥A−T∥<δ is Fredholm, and then ind⁡A=ind⁡T.

Facts & Assumptions

[A1]

A Fredholm T admits bounded projections splitting X=ker⁡T⊕X1 and Y=ran⁡T⊕Y0, with N:=ker⁡T and Y0 finite dimensional, dim⁡Y0=dim⁡coker⁡T, and with T1:=T∣X1:X1→ran⁡T a bounded isomorphism whose inverse T1−1 is bounded (Fredholm splitting and parametrix).

[A2]

Neumann: if ∥T1−1∥ ∥C∥<1 then T1+C is invertible with bounded inverse (Neumann series and small perturbations of bounded inverses, The operator norm as the least bound and as the unit-sphere or unit-ball supremum).

[A3]

Fredholm operators are closed under composition between Banach spaces and the index is additive, ind⁡(UT)=ind⁡U+ind⁡T (Fredholm index is additive, Fredholm operator cokernel and index); an invertible bounded operator is Fredholm with index 0, its kernel and cokernel being {0}.

[A4]

A linear map defined on a finite-dimensional normed space is bounded (A linear map from a finite-dimensional normed space is bounded); rank-nullity (Rank-nullity: dim⁡FV=nullity⁡T+rank⁡T, Finite-dimensional vector space, and its dimension dim⁡FV; infinite-dimensional means having no finite basis); and for a block-diagonal operator diag⁡(A11,S) on ran⁡T⊕Y0 the kernel is ker⁡A11⊕ker⁡S and the cokernel is isomorphic to coker⁡A11⊕coker⁡S (The quotient vector space (X/M), its cosets, and the quotient map (q:X\to X/M), Linear subspace of a vector space).

Proof

technique · direct

Given: AC, Banach spaces X,Y over one scalar field, a Fredholm T:X→Y, and the splitting X=N⊕X1, Y=ran⁡T⊕Y0 of [A1].

1.1A1

The projections PN, PX1, Pran⁡T, PY0 of the two splittings are bounded; write κ:=max⁡(1,∥Pran⁡T∥,∥PY0∥).

1.2A1A4

If X1={0}, then ran⁡T={0}, so X=N and Y=Y0 are finite dimensional, T=0, and for every bounded A:X→Y rank-nullity gives ind⁡A=dim⁡ker⁡A−dim⁡coker⁡A=dim⁡X−dim⁡Y=ind⁡T; so the claim holds with any δ>0 in this case.

2.1step 1.1A1A2algebra

Assume X1≠{0}, so ran⁡T≠{0} and ∥T1−1∥>0, and put δ:=1/(2κ∥T1−1∥)>0. For every bounded A with ∥A−T∥<δ, writing A11=Pran⁡TA∣X1 and T11=T1 one has ∥A11−T1∥≤κ∥A−T∥, so ∥T1−1(A11−T1)∥<1/2<1 and A11=T1(I+T1−1(A11−T1)) is invertible with bounded inverse by [A2].

3.1step 1.1step 2.1A1algebra

Under the hypothesis of [step 2.1], reorder the domain splitting as X=X1⊕N and keep the codomain splitting Y=ran⁡T⊕Y0. Let U:Y→Y and V:X→X be the bounded operators whose block matrices in these stated orders are U=(Iran⁡T0−A21A11−1IY0) and V=(IX1−A11−1A120IN), where A12=Pran⁡TA∣N, A21=PY0A∣X1 and A22=PY0A∣N; then UAV=diag⁡(A11,S) with S:=A22−A21A11−1A12, and U,V are invertible with bounded inverses given by the same matrices with the off-diagonal signs reversed.

4.1step 3.1A4

Under the hypothesis of [step 2.1], UAV=diag⁡(A11,S) is Fredholm with index ind⁡(UAV)=ind⁡A11+ind⁡S=ind⁡S, because A11 is an isomorphism of X1 onto ran⁡T and S maps the finite-dimensional space N boundedly into the finite-dimensional space Y0; by [A4] its index is ind⁡S=dim⁡ker⁡S−dim⁡coker⁡S=dim⁡ker⁡S+dim⁡im⁡S−dim⁡Y0=dim⁡N−dim⁡Y0.

5.1step 3.1step 4.1A3

Under the hypothesis of [step 2.1], A is Fredholm with ind⁡A=dim⁡N−dim⁡Y0=ind⁡T: since U,V and their inverses are invertible hence Fredholm of index 0, [A3] gives first that A=U−1(UAV)V−1 is Fredholm, and then ind⁡A=ind⁡(U−1)+ind⁡(UAV)+ind⁡(V−1)=ind⁡(UAV).

6.1step 1.2step 5.1∎

In the case of [step 1.2] and in the case of [step 5.1] every bounded A with ∥A−T∥ below the corresponding δ (any positive number in the first case, the δ of [step 2.1] in the second) is Fredholm of index ind⁡T, so the Fredholm operators are open in B(X,Y) and the index is locally constant at T.

Depends on

Dependency tree · 2 levels

Sources