Homemath.CVarXiv:2605.30114

On the coefficient formula for de Branges-Rovnyak norms

math.CVmath.FA2026-05v1license

Abstract

Let H(b)\mathcal{H}(b) be the de Branges-Rovnyak space associated to a non-extreme point bb of the unit ball of HH^\infty, and let ϕ=b/a\phi=b/a, where aa is the Pythagorean mate of bb. It is known that, if ff is a function holomorphic on a neighbourhood of the closed unit disk, then it belongs to H(b)\mathcal{H}(b), and its norm in H(b)\mathcal{H}(b) can be expressed in terms of the Taylor coefficients of ff and ϕ\phi via the formula fH(b)2=m0f^(m)2+m0n0ϕ^(n)f^(m+n)2. \|f\|_{\mathcal{H}(b)}^2=\sum_{m\ge0}|\hat{f}(m)|^2 +\sum_{m\ge0}\Bigl|\sum_{n\ge0}\overline{\hat{\phi}(n)}\hat{f}(m+n)\Bigr|^2. However, the formula can break down for some other fH(b)f\in\mathcal{H}(b). In this article we extend the scope of the formula to all fH2f\in H^2 for which the right-hand side is finite, provided that either ϕH2\phi\in H^2 or ϕ\phi is rational. If merely ϕHp\phi\in H^p for some p(0,2]p\in(0,2], then the formula still holds provided that, in addition, m0m2/p1f^(m)2<\sum_{m\ge0}m^{2/p-1}|\hat{f}(m)|^2<\infty. We also establish a limit-form of the formula that is valid for all non-extreme bb and all fH(b)f\in\mathcal{H}(b).

Comments: 18 pages

Cite

@article{arxiv.2605.30114,
  title  = {On the coefficient formula for de Branges-Rovnyak norms},
  author = {Thomas Ransford},
  journal= {arXiv preprint arXiv:2605.30114},
  year   = {2026}
}