We develop a theory of regularity for continuum Schrödinger operators
based on the Martin compactification of the complement of the essential
spectrum. This theory is inspired by Stahl–Totik regularity for orthogonal
polynomials, but requires a different approach, since Stahl–Totik regularity is
formulated in terms of the potential-theoretic Green’s function with a pole at
,
logarithmic capacity, and the equilibrium measure, notions which do not extend to
unbounded spectra. For any half-line Schrödinger operator with a bounded potential (in
a locally
sense), we prove that its essential spectrum obeys the
Akhiezer–Levin condition, and moreover, that the Martin function at
obeys the two-term
asymptotic expansion
as
. The
constant
in that expansion has not appeared in the literature before; we show that it
can be used to measure the size of the spectrum in a potential-theoretic
sense and that it should be thought of as a renormalized Robin constant
suited for semibounded sets. We prove that it enters a universal inequality
,
which leads to a notion of regularity, with connections to the root asymptotics of
Dirichlet solutions and zero counting measures. We also present applications to
decaying and ergodic potentials.