Correct radial operator
Consider the scalar operator on ordinary , , in units . For a normalized spherical harmonic with angular eigenvalue , write and . This transformation sends the radial norm to . Differentiating yields
The term is contributed by the radial measure. Use the Friedrichs realization inherited from the full spatial quadratic form. In particular the regular branch has ; the critical endpoint selects the regular, nonlogarithmic branch. An arbitrary half-line boundary condition describes a different operator.
A form bound on attraction
For , integration by parts for smooth compactly supported gives
Choose and extend by form closure:
This is Hardy's inequality; see Nonnenmacher, Proposition 3.2.7.
As an application, measure lengths in a stated range and energies in . For the dimensionless operator
subtract its limiting potential . Since ,
Thus excludes every spectral value below . The bound is sufficient; exceeding it alone does not establish a bound state. A first-order Dirac operator needs its own analysis.
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Confining oscillator domain — treats an unbounded harmonic potential with compact resolvent.
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Coulomb exponential profiles — illustrates how normalized spatial profiles enter energy bounds.
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Resonance and profile tools — overview and verification.
resonance_profile_checks.py checks finite examples by quadrature, matrix evolution, and independent algebra.