2004
DOI: 10.2140/pjm.2004.215.297
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Lq-theory of a singular “winding” integral operator arising from fluid dynamics

Abstract: We analyze in classical L q (R n )-spaces, n = 2 or n = 3, 1 < q < ∞, a singular integral operator arising from the linearization of a hydrodynamical problem with a rotating obstacle. The corresponding system of partial differential equations of second order involves an angular derivative which is not subordinate to the Laplacian. The main tools are LittlewoodPaley theory and a decomposition of the singular kernel in Fourier space.

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Cited by 71 publications
(78 citation statements)
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“…The spaceŴ k,q (Ω) consists of equivalence classes of L 1 loc -functions being unique only up to elements from Π k−1 and is equipped with the norm |α|=k ∂ α u q , where · q denotes the L q -norm. However, sometimes being less careful, we will consider v ∈Ŵ k,q (Ω) as a function (representative) rather than an equivalence class of functions, i.e., v ∈ L 1 loc (Ω) such that ∂ α v ∈ L q (Ω) for every multi-index α with |α| = k. For further results on similar problems we refer to [4], [8], [9], [10], [11], [12] and [13].…”
mentioning
confidence: 99%
“…The spaceŴ k,q (Ω) consists of equivalence classes of L 1 loc -functions being unique only up to elements from Π k−1 and is equipped with the norm |α|=k ∂ α u q , where · q denotes the L q -norm. However, sometimes being less careful, we will consider v ∈Ŵ k,q (Ω) as a function (representative) rather than an equivalence class of functions, i.e., v ∈ L 1 loc (Ω) such that ∂ α v ∈ L q (Ω) for every multi-index α with |α| = k. For further results on similar problems we refer to [4], [8], [9], [10], [11], [12] and [13].…”
mentioning
confidence: 99%
“…In particular, we shall give simple proofs of certain L q -estimates originally established by Farwig, Hishida, and Müller in [9] and by Farwig in [6].…”
Section: Flow Past a Rotating Bodymentioning
confidence: 90%
“…Maximal regularity in an L q -setting of the system (3.88) was established for the first time in the Stokes case (λ = 0) by Farwig, Hishida, and Müller in [9], and in the Oseen case (λ = 0) by Farwig in [6]. More specifically, in [9, Theorem 1.1] the following result was obtained:…”
Section: Flow Past a Rotating Bodymentioning
confidence: 95%
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