Definition
A bounded linear map between Banach spaces whose kernel and cokernel are finite-dimensional and whose range is closed; its index is dim(kernel) minus dim(cokernel).

Principle

Principle
Fredholm property is stable under compact perturbations and the index is an integer invariant under such perturbations.

Demonstration

Demonstration
An integral operator on L^2 with a smooth kernel defines a Fredholm operator: its kernel and cokernel are finite-dimensional and the index can be computed from boundary data.

Misapplication

Misapplication
Calling any bounded operator with closed range a Fredholm operator without checking finite-dimensionality of kernel or cokernel.

Consequence

Consequence
Equations of the form T x = y are solvable up to a finite-dimensional obstruction; solvability reduces to finitely many compatibility conditions and a uniquely determined solution modulo ker(T).

Reversal

Reversal
A non-Fredholm operator typically has an infinite-dimensional kernel or cokernel or a non-closed range; such operators lack a well-defined finite index.

Boundary

Boundary
This concept applies to bounded linear operators on Banach (or Hilbert) spaces; unbounded operators require additional closedness and domain conditions and are treated separately.

Semantic Tension

Semantic Tension
Often contrasted with compact operators (which have discrete spectrum accumulating at zero) and with invertible operators; Fredholmness is weaker than invertibility but stronger than mere boundedness.

Synthesis

Synthesis
A Fredholm operator is a bounded linear operator between Banach spaces with finite-dimensional defect spaces and closed range, yielding a stable integer index under compact perturbations.