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The Fourier formula for discontinuous functions of several variables

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THE FOURIER FORMULA FOR DISCONTINUOUS<br />

FUNCTIONS OF SEVERAL VARIABLES<br />

A.N. Podkorytov and Mai Van Minh<br />

We would like to talk about following problem. Suppose Ω is convex compact<br />

set in R m and χ Ω its indicator. Obviously its <strong>Fourier</strong> trans<strong>for</strong>mation ̂χ Ω is not<br />

summable in R m , if Int(Ω) ≠ ∅. <strong>The</strong> problem is to interpret the integral in the<br />

R.H.S. <strong>of</strong> the <strong>of</strong> inversion <strong><strong>for</strong>mula</strong><br />

∫<br />

χ Ω (y 0 ) = ̂χ Ω (x)e −2πix·y0 dx,<br />

R m<br />

while keeping the equality true. For example if Ω = □ = [a 1 , b 1 ] × . . . × [a m , b m ] is<br />

a rectangular parallelepiped it is not hard to verify that<br />

∫<br />

̂χ □ (x)e −2πix·y0 dx −→ χ □ (y 0 ) <strong>for</strong> y 0 /∈ ∂□.<br />

[−R,R] m R→+∞<br />

But as mentioned in [1], if Ω = ○ = {y ∈ R m | ‖y‖ ≤ 1} is a sphere then the<br />

situation becomes more complicated. If y 0 ≠ 0 then<br />

∫<br />

̂χ ○ (x)e −2πix·y0 dx −→ χ ○ (y) <strong>for</strong> y 0 /∈ ∂○<br />

R→+∞<br />

‖x‖≤R<br />

(in case ‖y 0 ‖ = 1 the limit equals 1 2 ). At the same time when m ≥ 3 at y 0 = 0 these<br />

integrals do not have a limit. In [2] the sphere {‖x‖ ≤ R} have been replaced by a<br />

cube and it has been ∫ shown that when m = 3 and y 0 = 0 the following equality is<br />

correct 1 = lim ̂χ<br />

R→+∞<br />

[−R,R] 3 ○ (x) dx. In order to extend this result, we could prove<br />

that <strong>for</strong> every convex compact set Ω ⊂ R m , m ≥ 2, the following equality is correct<br />

∫<br />

χ Ω (y 0 ) =<br />

̂χ Ω (x)e −2πix·y0 dx <strong>for</strong> y 0 /∈ ∂Ω,<br />

lim<br />

R→+∞<br />

x∈RW<br />

if W is polyhedron in R m , 0 ∈ Int(W ) and the sides <strong>of</strong> W and their extensions do<br />

not cross the origin. If m = 2 we can take as W any compact convex neighborhood<br />

<strong>of</strong> the origin instead <strong>of</strong> polygon. In this case the inversion <strong><strong>for</strong>mula</strong> remains the<br />

same <strong>for</strong> y 0 /∈ ∂Ω. And, what is more interesting, if W is simmetrical (relatively<br />

the origin) at every point <strong>of</strong> y 0 ∈ ∂Ω there is finite limit <strong>of</strong> integrals on RW . It<br />

equals 1 2 , if y 0 is not boundary angular point (vertex). For boundary angular point<br />

this limits depends on choice <strong>of</strong> W .<br />

[1] Pinsky M. A., Stanton N. K., Trapa P. E. <strong>Fourier</strong> series <strong>of</strong> radial <strong>functions</strong><br />

in <strong>several</strong> <strong>variables</strong>. J. Funct. Anal. 1993. V. 116. P. 111 – 122.<br />

1<br />

Typeset by AMS-TEX


2 A.N. PODKORYTOV AND MAI VAN MINH<br />

[2] Harada C., Nakai E. <strong>The</strong> square partial sums <strong>of</strong> the <strong>Fourier</strong> trans<strong>for</strong>m <strong>of</strong><br />

radial <strong>functions</strong> in three dimensions. Sc. Math. Japon. 2002. V. 55, No. 3. P. 467<br />

– 477.<br />

[3] Podkorytov A.N., Mai Van Minh. <strong>The</strong> <strong>Fourier</strong> <strong><strong>for</strong>mula</strong> <strong>for</strong> <strong>discontinuous</strong><br />

<strong>functions</strong> <strong>of</strong> <strong>several</strong> <strong>variables</strong>. J. Math. Sci. 2004. Vol. 124. No. 3. P. 5018 –<br />

5025.<br />

[4] Mai Van Minh. <strong>The</strong> <strong>Fourier</strong> integral <strong>for</strong> <strong>discontinuous</strong> <strong>functions</strong> <strong>of</strong> two <strong>variables</strong>.<br />

Vestnik S.-Peterburgskogo univ. 2006. Ser. 1. No. 1. P. 45 – 49.

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