The Lebesgue constant for the periodic Franklin system

Markus Passenbrunner

Studia Mathematica (2011)

  • Volume: 205, Issue: 3, page 251-279
  • ISSN: 0039-3223

Abstract

top
We identify the torus with the unit interval [0,1) and let n,ν ∈ ℕ with 0 ≤ ν ≤ n-1 and N:= n+ν. Then we define the (partially equally spaced) knots t j = ⎧ j/(2n) for j = 0,…,2ν, ⎨ ⎩ (j-ν)/n for for j = 2ν+1,…,N-1. Furthermore, given n,ν we let V n , ν be the space of piecewise linear continuous functions on the torus with knots t j : 0 j N - 1 . Finally, let P n , ν be the orthogonal projection operator from L²([0,1)) onto V n , ν . The main result is l i m n , ν = 1 | | P n , ν : L L | | = s u p n , 0 ν n | | P n , ν : L L | | = 2 + ( 33 - 18 3 ) / 13 . This shows in particular that the Lebesgue constant of the classical Franklin orthonormal system on the torus is 2 + (33-18√3)/13.

How to cite

top

Markus Passenbrunner. "The Lebesgue constant for the periodic Franklin system." Studia Mathematica 205.3 (2011): 251-279. <http://eudml.org/doc/285864>.

@article{MarkusPassenbrunner2011,
abstract = {We identify the torus with the unit interval [0,1) and let n,ν ∈ ℕ with 0 ≤ ν ≤ n-1 and N:= n+ν. Then we define the (partially equally spaced) knots $t_\{j\}$ = ⎧ j/(2n) for j = 0,…,2ν, ⎨ ⎩ (j-ν)/n for for j = 2ν+1,…,N-1. Furthermore, given n,ν we let $V_\{n,ν\}$ be the space of piecewise linear continuous functions on the torus with knots $\{t_\{j\}: 0 ≤ j ≤ N-1\}$. Finally, let $P_\{n,ν\}$ be the orthogonal projection operator from L²([0,1)) onto $V_\{n,ν\}$. The main result is $lim_\{n→∞,ν=1\} ||P_\{n,ν\}: L^\{∞\} → L^\{∞\}|| = sup_\{n∈ℕ,0≤ν≤n\} ||P_\{n,ν\}: L^\{∞\} → L^\{∞\}|| = 2 + (33-18√3)/13$. This shows in particular that the Lebesgue constant of the classical Franklin orthonormal system on the torus is 2 + (33-18√3)/13.},
author = {Markus Passenbrunner},
journal = {Studia Mathematica},
keywords = {periodic Franklin system; Lebesgue constant},
language = {eng},
number = {3},
pages = {251-279},
title = {The Lebesgue constant for the periodic Franklin system},
url = {http://eudml.org/doc/285864},
volume = {205},
year = {2011},
}

TY - JOUR
AU - Markus Passenbrunner
TI - The Lebesgue constant for the periodic Franklin system
JO - Studia Mathematica
PY - 2011
VL - 205
IS - 3
SP - 251
EP - 279
AB - We identify the torus with the unit interval [0,1) and let n,ν ∈ ℕ with 0 ≤ ν ≤ n-1 and N:= n+ν. Then we define the (partially equally spaced) knots $t_{j}$ = ⎧ j/(2n) for j = 0,…,2ν, ⎨ ⎩ (j-ν)/n for for j = 2ν+1,…,N-1. Furthermore, given n,ν we let $V_{n,ν}$ be the space of piecewise linear continuous functions on the torus with knots ${t_{j}: 0 ≤ j ≤ N-1}$. Finally, let $P_{n,ν}$ be the orthogonal projection operator from L²([0,1)) onto $V_{n,ν}$. The main result is $lim_{n→∞,ν=1} ||P_{n,ν}: L^{∞} → L^{∞}|| = sup_{n∈ℕ,0≤ν≤n} ||P_{n,ν}: L^{∞} → L^{∞}|| = 2 + (33-18√3)/13$. This shows in particular that the Lebesgue constant of the classical Franklin orthonormal system on the torus is 2 + (33-18√3)/13.
LA - eng
KW - periodic Franklin system; Lebesgue constant
UR - http://eudml.org/doc/285864
ER -

NotesEmbed ?

top

You must be logged in to post comments.

To embed these notes on your page include the following JavaScript code on your page where you want the notes to appear.

Only the controls for the widget will be shown in your chosen language. Notes will be shown in their authored language.

Tells the widget how many notes to show per page. You can cycle through additional notes using the next and previous controls.

    
                

Note: Best practice suggests putting the JavaScript code just before the closing </body> tag.