2019
DOI: 10.1142/s0129055x19500077
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A note on measures vanishing at infinity

Abstract: In this paper, we review the basic properties of measures vanishing at infinity and prove a version of the Riemann-Lebesgue lemma for Fourier transformable measures.2010 Mathematics Subject Classification. 43A25, 52C23.

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Cited by 4 publications
(4 citation statements)
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“…Proof (a)This follows from [34, Theorem 4.1] or [36, Theorem 5.7]. (b)This is a consequence of [29, Corollary 35]. (c)By Corollary 5.11, we have fWLS2(double-struckRd)$f \in \mathcal {WLS}_2({\mathbb {R}}^d)$. The claim follows now from Theorem 5.13.$\Box$ …”
Section: On the Components Of The Generalized Eberlein Decompositionmentioning
confidence: 91%
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“…Proof (a)This follows from [34, Theorem 4.1] or [36, Theorem 5.7]. (b)This is a consequence of [29, Corollary 35]. (c)By Corollary 5.11, we have fWLS2(double-struckRd)$f \in \mathcal {WLS}_2({\mathbb {R}}^d)$. The claim follows now from Theorem 5.13.$\Box$ …”
Section: On the Components Of The Generalized Eberlein Decompositionmentioning
confidence: 91%
“…Let us start with necessary conditions. Here, we follow the approach of [29, Theorem 27]. Proposition Let ωDTBM0a(double-struckRd)$\omega \in \mathcal {DTBM}_{\operatorname{0a}}({\mathbb {R}}^d)$.…”
Section: On the Components Of The Generalized Eberlein Decompositionmentioning
confidence: 99%
See 1 more Smart Citation
“…First, since a n are linearly independent, we have n + a n ≠ m + a m for all n ≠ m. Indeed, if we assume by contradiction that there exists some n ≠ m such that n + a n = m + a m then (m − n) ⋅ 1 + 1 ⋅ a m + (−1) ⋅ a n = 0 , contradicting the linear independence. It follows that δ Λ − δ Z is a measure vanishing at infinity, and hence null weakly almost periodic [32].…”
Section: Pure Point Diffractive Setsmentioning
confidence: 96%