English

The Lebesgue Constant for the Periodic Franklin System

Numerical Analysis 2015-03-04 v3

Abstract

We identify the torus with the unit interval [0,1)[0,1) and let n,νNn,\nu\in\mathbb{N}, 1νn11\leq \nu\leq n-1 and N:=n+νN:=n+\nu. Then we define the (partially equally spaced) knots tj={[c]ll t_{j}=\{[c]{ll}% \frac{j}{2n}, & \text{for}j=0,...,2\nu, \frac{j-\nu}{n}, & \text{for}j=2\nu+1,...,N-1.] Furthermore, given $n,\nu$ we let $V_{n,\nu}$ be the space of piecewise linear continuous functions on the torus with knots $\{t_j:0\leq j\leq N-1\}$. Finally, let $P_{n,\nu}$ be the orthogonal projection operator of $L^{2}([0,1))$ onto $V_{n,\nu}.$ The main result is \[\lim_{n\rightarrow\infty,\nu=1}\|P_{n,\nu}:L^\infty\rightarrow L^\infty\|=\sup_{n\in\mathbb{N},0\leq \nu\leq n}\|P_{n,\nu}:L^\infty\rightarrow L^\infty\|=2+\frac{33-18\sqrt{3}}{13}. This shows in particular that the Lebesgue constant of the classical Franklin orthonormal system on the torus is 2+33183132+\frac{33-18\sqrt{3}}{13}.

Keywords

Cite

@article{arxiv.1103.1950,
  title  = {The Lebesgue Constant for the Periodic Franklin System},
  author = {Markus Passenbrunner},
  journal= {arXiv preprint arXiv:1103.1950},
  year   = {2015}
}

Comments

Mathematica Notebook for creating Table 1 on page 21 is attached