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Rank-one resolvent and bound-state equation
Statement
Assume the Axiom of Choice. Let be a self-adjoint operator on a complex Hilbert space , with inner product linear in its first variable and . Let , , and define by . Put on and . Then is self-adjoint. For every such that , one has and For real and , is an eigenvalue of if and only if ; in that case the eigenspace is one-dimensional.
Statement references
Facts & Assumptions
Given: The self-adjoint lower-semibounded operator , its domain, , real , and the rank-one map defined in the Statement.
The resolvent set consists of those for which is bijective with bounded inverse; for self-adjoint , each real belongs to the resolvent set (Resolvent and spectrum of an unbounded operator, Resolvent of a self-adjoint operator: nonreal resolvents and the estimate).
Kato–Rellich: a symmetric perturbation with relative operator bound less than one preserves self-adjointness on the original operator domain (Kato-Rellich theorem).
Cauchy–Schwarz gives , and the inner product is linear in its first argument (Cauchy–Schwarz: , with equality exactly for dependent pairs, Real and complex inner-product spaces and their induced length).
Kato–Rellich assumes the Axiom of Choice; the self-adjoint resolvent input assumes Countable Choice. The stated AC hypothesis supplies the latter: for any sequence of nonempty sets, apply AC to to obtain a choice function ; then for every , which is Countable Choice (The Axiom of Choice).
Proof
Given: [A1], [A2], , and the operators in the Statement.
For every , [F2] gives . Also , so is bounded and self-adjoint, including . Thus is symmetric on with relative bound zero; [F1] implies that is self-adjoint on .
Fix and write , , and . Then and ; hence . If , direct multiplication gives .
Define . Its range is contained in . Since , on one has . On one has , using . Thus is a bounded two-sided inverse from onto , and its expansion is the stated resolvent formula.
Let be real. By [A1], exists. If with , then . The coefficient cannot be zero, because that would give ; applying therefore yields . Conversely, if this scalar is zero, then and . Every eigenvector satisfies the same scalar-multiple formula for , so the eigenspace is one-dimensional.