Alphabeta Math
CorollaryStatement: AI-adaptedProof: AI-generatedprecheck passaudited 2026-08-31
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  • 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.
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For a Hermitian simple eigenvalue, one may take y=x and the first-order formulas simplify accordingly

Statement

If A(t) is a differentiable Hermitian matrix path, and λ(t),x(t) is a differentiable simple eigenpair branch with ∥x(t)∥2=1, then one may choose the phase locally so that x(t)∗x′(t)=0. With that choice,

λ′(t)=x(t)∗A′(t)x(t),x′(0)=−SA′(0)x(0).

Facts & Assumptions

Given: A differentiable Hermitian matrix path A(t) and a differentiable simple unit eigenvector branch x(t).

Proof

technique · direct
1.1givenalgebra

If A(t)=A(t)∗ and A(t)x(t)=λ(t)x(t), then taking adjoints shows x(t)∗A(t)=λ(t)x(t)∗. Thus the same unit eigenvector can serve as both left and right eigenvector. Multiplying x(t) by a unit complex phase if necessary imposes the gauge x(t)∗x′(t)=0.

2.1L1step 1.1∎

Substitute y=x into the formulas summarized in [L1]. This gives λ′(t)=x(t)∗A′(t)x(t) and, in the chosen gauge, x′(0)=−SA′(0)x(0).

Depends on

Used by

Dependency tree · two levels

7 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources