2004
DOI: 10.1017/s0027763000008734
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A global theory of flexes of periodic functions

Abstract: Abstract. For a real valued periodic smooth function u on R, n ≥ 0, one defines the osculating polynomial ϕs (of order 2n + 1) at a point s ∈ R to be the unique trigonometric polynomial of degree n, whose value and first 2n derivatives at s coincide with those of u at s. We will say that a point s is a clean maximal flex (resp. clean minimal flex ) of the function u on S 1 if and only if ϕs ≥ u (resp. ϕs ≤ u) and the preimage (ϕ − u) −1 (0) is connected. We prove that any smooth periodic function u has at leas… Show more

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Cited by 9 publications
(13 citation statements)
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References 10 publications
(15 reference statements)
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“…A similar result is proved in [17] and [18] for clean sextactic points on a strictly convex curve in the affine plane. It says that such a curve has three inscribed osculating conics and three circumscribed osculating conics.…”
Section: Figure 4 a Simple Closed Curve With No Clean Inflection Pointssupporting
confidence: 77%
See 1 more Smart Citation
“…A similar result is proved in [17] and [18] for clean sextactic points on a strictly convex curve in the affine plane. It says that such a curve has three inscribed osculating conics and three circumscribed osculating conics.…”
Section: Figure 4 a Simple Closed Curve With No Clean Inflection Pointssupporting
confidence: 77%
“…Then A m is the kernel of the operator L m . The following proposition is proved in the appendix of [18], p. 135. A function f : R → R is called π-antiperiodic if it satisfies f (t + π) = −f (t).…”
Section: Anti-periodic Functions and Curves Of Constant Widthmentioning
confidence: 92%
“…See Example (i) that we give after the axioms and the next section for full details of this application. Generalizations to higher order intrinsic systems and applications to Fourier series of periodic functions will be given in [TU2]. We explain a special case of the construction in [TU2] in Example (ii) after the axioms.…”
Section: B Intrinsic Conic Systemsmentioning
confidence: 99%
“…(ii) For a real valued C 4 -function u on S 1 , one defines the osculating polynomial ϕ s (of order five) at a point s ∈ S 1 to be the unique trigonometric polynomial of degree two, ϕ s (t) = a 0 + a 1 cos t + b 1 sin t + a 2 cos 2t + b 2 sin 2t, whose value and first four derivatives at s coincide with those of u at s. If u is C 5 and the value and the first five derivatives of u and ϕ s coincide in s, i.e., if ϕ s hyperosculates u in s, then we call s a flex of u (of order five). The existence of six flexes of order five can easily be proved as a consequence of the well-known fact that a function has at least six zeros if its Fourier coefficients a i and b i vanish for i ≤ 2, see [TU2]. One can use intrinsic conic systems to prove the much stronger result that there are six such flexes satisfying the global property that the osculating polynomials ϕ s in the flexes support u, i.e., either ϕ s ≤ u or u ≤ ϕ s .…”
Section: B Intrinsic Conic Systemsmentioning
confidence: 99%
“…Of recent results, we would like to mention [60] in which the Sturm theorem is extended from Fourier series to Fourier integrals and [218] where analogs of extactic points for trigonometric polynomials are studied.…”
Section: Commentmentioning
confidence: 99%