English

On the singular value decomposition of n-fold integration operators

Numerical Analysis 2020-02-11 v1 Spectral Theory

Abstract

In theory and practice of inverse problems, linear operator equations Tx=yTx=y with compact linear forward operators TT having a non-closed range R(T)\mathcal{R}(T) and mapping between infinite dimensional Hilbert spaces plays some prominent role. As a consequence of the ill-posedness of such problems, regularization approaches are required, and due to its unlimited qualification spectral cut-off is an appropriate method for the stable approximate solution of corresponding inverse problems. For this method, however, the singular system {σi(T),ui(T),vi(T)}i=1\{\sigma_i(T),u_i(T),v_i(T)\}_{i=1}^\infty of the compact operator TT is needed, at least for i=1,2,...,Ni=1,2,...,N, up to some stopping index NN. In this note we consider nn-fold integration operators T=Jn  (n=1,2,...)T=J^n\;(n=1,2,...) in L2([0,1])L^2([0,1]) occurring in numerous applications, where the solution of the associated operator equation is characterized by the nn-th generalized derivative x=y(n)x=y^{(n)} of the Sobolev space function yHn([0,1])y \in H^n([0,1]). Almost all textbooks on linear inverse problems present the whole singular system {σi(J1),ui(J1),vi(J1)}i=1\{\sigma_i(J^1),u_i(J^1),v_i(J^1)\}_{i=1}^\infty in an explicit manner. However, they do not discuss the singular systems for Jn,  n2J^n,\;n \ge 2. We will emphasize that this seems to be a consequence of the fact that for higher nn the eigenvalues σi2(Jn)\sigma^2_i(J^n) of the associated ODE boundary value problems obey transcendental equations, the complexity of which is growing with nn. We present the transcendental equations for n=2,3,...n=2,3,... and discuss and illustrate the associated eigenfunctions and some of their properties.

Keywords

Cite

@article{arxiv.1811.11642,
  title  = {On the singular value decomposition of n-fold integration operators},
  author = {Ronny Ramlau and Christoph Koutschan and Bernd Hofmann},
  journal= {arXiv preprint arXiv:1811.11642},
  year   = {2020}
}
R2 v1 2026-06-23T06:23:46.793Z