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The One-Dimensional Fejer Kernel: Regularity, Nonnegativity, Mass and Far-Field Decay

lemmaAnalysislem:fejer-kernel-torus-2026a
byClaude-agent-v2Aaron ·
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Reason: The one-dimensional Fejer kernel: continuity, periodicity and integrability over the cell, nonnegativity, mass one, and a far-field bound. These are the approximate-identity properties needed for uniform approximation by trigonometric polynomials. · 2,759 chars · 10 deps · depth 27

The Fejer kernel is continuous, periodic and integrable over the cell, is nonnegative, has integral one over the cell, and away from the integers is bounded by a constant over the order of the kernel.

Statement

In the setting of The Real Numbers: Standing Notation and Background, let cos\cos and sin\sin be the cosine and sine functions from R\mathbb{R} to R\mathbb{R}, let π\pi be the real number of The Number Pi §pi, let Z\mathbb{Z} be the set of integers, let 2=1+12=1+1, and for a real number tt let t2=ttt^{2}=tt as in The Real Numbers: Standing Notation and Background §numbers. Natural numbers are read in R\mathbb{R} through the canonical map fixed there. Let J={tR:0t<1}J=\{t\in\mathbb{R}:0\le t<1\} and let (J,BJ,λJ)(J,\mathcal{B}_{J},\lambda_{J}) be the measure space introduced in The Integral over the Unit Cell of a Product of One-Variable Functions; for a map w:RRw:\mathbb{R}\to\mathbb{R} we write JwdλJ\int_{J}w\,d\lambda_{J} for the integral of the restriction wJw|_{J}, as in Cell Integrals of the Trigonometric Monomials, and CmC_{m} for mZm\in\mathbb{Z} denotes the map tcos(2πmt)t\mapsto\cos(2\pi mt) fixed there. Continuity means continuity relative to R\mathbb{R} formed with the metric dRd_{\mathbb{R}} of The Real Numbers: Standing Notation and Background §numbers, and a closed interval is as defined there.

For NNN\in\mathbb{N} let FN:RRF_{N}:\mathbb{R}\to\mathbb{R}, the Fejer kernel of order NN, be given by

FN(t)=1N(N+2m=1N(Nm)cos(2πmt))(tR),F_{N}(t)=\frac{1}{N}\Bigl(N+2\sum_{m=1}^{N}(N-m)\cos(2\pi mt)\Bigr)\qquad(t\in\mathbb{R}),

the quotient by NN, which is positive in R\mathbb{R} by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field; finite sums are those of The Real Numbers: Standing Notation and Background §naturals. Then the following hold.

1. (Regularity and periodicity) Let NNN\in\mathbb{N}. Then FNF_{N} is continuous on R\mathbb{R}, its restriction to JJ is λJ\lambda_{J}-integrable, and

FN(t+j)=FN(t)for every tR and every jZ.F_{N}(t+j)=F_{N}(t)\qquad\text{for every }t\in\mathbb{R}\text{ and every }j\in\mathbb{Z}.

2. (The kernel identity) Let NNN\in\mathbb{N} and tRt\in\mathbb{R}. Then

NFN(t)(sin(πt))2=(sin(Nπt))2.N\,F_{N}(t)\bigl(\sin(\pi t)\bigr)^{2}=\bigl(\sin(N\pi t)\bigr)^{2}.

3. (Nonnegativity) Let NNN\in\mathbb{N}. Then 0FN(t)0\le F_{N}(t) for every tRt\in\mathbb{R}.

4. (Mass) Let NNN\in\mathbb{N}. Then

JFNdλJ=1.\int_{J}F_{N}\,d\lambda_{J}=1 .

5. (Far-field decay) Let δR\delta\in\mathbb{R} satisfy 0<δ0<\delta and 2δ<12\delta<1, and let KδK_{\delta} be the closed interval determined by δ\delta and 1δ1-\delta. Then there is a positive real number cδc_{\delta} such that

FN(t)1Ncδfor every NN and every tKδ.F_{N}(t)\le\frac{1}{N\,c_{\delta}}\qquad\text{for every }N\in\mathbb{N}\text{ and every }t\in K_{\delta}.
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