Example. A transfer norm greater than one [fdip-007X]

Take \(w=3/2\) and \(m^2=4/5\) in Theorem [fdip-007U]. Then \[\begin {aligned} \cosh \omega &=\frac {19}{15},& s&=\frac {\sqrt {34}}5,\\ q&=\frac {19-2\sqrt {34}}{15},& \lambda _0&=\sqrt {\frac {4\pi q}{3}}. \end {aligned}\] Numerically \(\omega \approx 0.714971\) and \(\lambda _0\approx 1.431497\). In particular \(\|T\|=\lambda _0>1\). This inequality does not depend on rounding: \(\sqrt {34}<6\) gives \(q>7/15\), and \(\pi >3\) gives \(\lambda _0^2>28/15>1\).

All eigenvalues are nevertheless positive: \(\lambda _n=\lambda _0q^n\). Dividing by the leading eigenvalue gives \(\widehat T h_n^s=q^nh_n^s\) and \(\|\widehat T\|=1\). The lowest mode label \(n=0\) refers to the Gaussian function \(h_0^s\), not to a constant function on \(\mathbb R\); the latter does not belong to Lebesgue \(L^2\). Thus the normalization is a genuine scalar factor in the operator, fixed by the chosen reference measure.