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TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-5.6-terra)audited 2026-09-04
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  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
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Lebesgue constants grow logarithmically

Statement

There are absolute constants c,C>0 such that, for every N1,

clog(N+1)01DN(t)dtClog(N+1).

Facts & Assumptions

Given: An integer N1.

[L1]

For tZ, DN(t)=sin((2N+1)πt)sin(πt), and in particular DN(1t)=DN(t) for 0<t<1 (Closed form and size bounds for the Dirichlet kernel).

Proof

technique · direct
1.1

For 0<t<1, [L1] gives DN(1t)=DN(t), so 01DN(t)dt=201/2DN(t)dt. Split the last integral at 1/(2N+1). On (0,1/(2N+1)], [L1] and the bound DN(t)2N+1 give a contribution at most 1. On [1/(2N+1),1/2], one has 0<πtπ/2<2, so [L2] implies sin(πt)πt/3. Using [L1], DN(t)1sin(πt)3πt. Therefore 01DN(t)dt2+6π1/(2N+1)1/2dttClog(N+1) for a universal C.

L1L2algebra
1.2

For m=0,,N1, let Jm:=[m+1/62N+1,m+5/62N+1]. These intervals lie in (0,1/2) and are disjoint. If tJm, then (2N+1)πt[(m+1/6)π,(m+5/6)π], so sin((2N+1)πt)1/2. Also sin(πt)πt. Hence [L1] gives DN(t)12πt(tJm).

L1algebra
2.1

Integrating the lower bound from step 1.2 over each Jm and summing yields 01/2DN(t)dt12πm=0N1Jmdtt=12πm=0N1log ⁣(m+5/6m+1/6). Since log ⁣(m+5/6m+1/6)2/3m+5/623(m+1), one gets 01/2DN(t)dt13πm=0N11m+113π1N+1dtt=13πlog(N+1). Using step 1.1 once more, 01DN(t)dt23πlog(N+1).

step 1.1step 1.2algebra
3.1

Steps 1.1 and 2.1 give the two-sided logarithmic bound.

step 1.1step 2.1

Depends on

Used by

Nothing in the library uses this result yet.

Dependency tree · two levels

7 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources