2017
DOI: 10.1007/s00209-017-1944-6
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The small-convection limit in a two-dimensional chemotaxis-Navier–Stokes system

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Cited by 48 publications
(28 citation statements)
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“…In order to successfully extract a uniform stabilization for n (κ) ε and u (κ) ε in certain L p spaces we will require the following auxiliary lemma for ODEs, which we have taken from [26,Lemma 4.3].…”
Section: Lemma 55mentioning
confidence: 99%
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“…In order to successfully extract a uniform stabilization for n (κ) ε and u (κ) ε in certain L p spaces we will require the following auxiliary lemma for ODEs, which we have taken from [26,Lemma 4.3].…”
Section: Lemma 55mentioning
confidence: 99%
“…for large η > 0 independent of κ ∈ [−1, 1] to derive, after a some bootstrapping, κ-independent bounds in C 1 Ω × C 2 Ω × D(A α ) uniform in time. These bounds, when combined with decay properties of (Λ κ ), then become the driving force of the exponential stabilization featured in [26]. In stark contrast, in the current three-dimensional framework we cannot utilize a corresponding quasi-energy functional immediately, as for (Λ κ ) only the global existence of a weak solution obtained by a limiting procedure from approximating systems is known ( [30]).…”
Section: Introductionmentioning
confidence: 98%
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“…As an immediate byproduct, the authors also obtained the usual L p − L 2 (1 ≤ p ≤ 2) type of the decay rates without requiring that the L p norm of initial data is small. For more details, one can refer to previous studies [15][16][17][18][19][20][21][22][23][24][25] and the reference therein.…”
Section: Introductionmentioning
confidence: 99%