Stability of good quantum numbers in ground states

Abstract

Let H be a self-adjoint operator, bounded from below and let O be a bounded self-adjoint operator with purely discrete spectrum. Suppose that (i) E(H)=∈f spec(H) is a simple eigenvalue, and (ii) H strongly commutes with O. Let H be the eigenvector associated with E(H). By the assumptions (i) and (ii), H is an eigenvector of O: OH=μ(H)H. In the context of quantum mechanics, μ(H) is called a good quantum number. In this note, we examine the stability of μ(H) under perturbations of H from a viewpoint of the order theory.

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