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Behavior of Solutions of Convolution Equation at Infinity

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Integral Geometry and Convolution Equations
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Abstract

Let ϕɛ′(ℝn), ϕ ≠ 0 and fL loc(ℝn) be a nonzero function satisfying the equation

$$ \left( {f * \phi } \right)\left( x \right) = 0, x \in \mathbb{R}^n . $$
(3.1)

Then f cannot decrease rapidly on infinity. For instance, if fL(ℝn), from (3.1), (1.6.2) we have \(\widehat f \cdot \widehat \varphi = 0\). Since \(\widehat \varphi\) is an entire function the set \(\{ x \in {\mathbb{R}^n}:\widehat \varphi (x) = 0\}\) is dense nowhere in ℝn. As \(\widehat f\) is continuous we obtain f = 0.

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© 2003 Springer Science+Business Media Dordrecht

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Volchkov, V.V. (2003). Behavior of Solutions of Convolution Equation at Infinity. In: Integral Geometry and Convolution Equations. Springer, Dordrecht. https://doi.org/10.1007/978-94-010-0023-9_16

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  • DOI: https://doi.org/10.1007/978-94-010-0023-9_16

  • Publisher Name: Springer, Dordrecht

  • Print ISBN: 978-94-010-3999-4

  • Online ISBN: 978-94-010-0023-9

  • eBook Packages: Springer Book Archive

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