2022
DOI: 10.1007/s00033-022-01677-0
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On the generalized Magnetohydrodynamics-$$\alpha $$ equations with fractional dissipation in Lei–Lin and Lei–Lin–Gevrey spaces

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Cited by 3 publications
(6 citation statements)
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“…where u(x, t) = (u 1 (x, t), u 2 (x, t), u 3 (x, t)) ∈ R 3 denotes the incompressible velocity field, and p(x, t) ∈ R the hydrostatic pressure; see [1,2,3,4,5,6,7,8,10,11,12,13,18,20,26,28,31] and their references. Here (−∆) α , with α ≥ 1/2, is the fractional Laplacian, see (2.1).…”
Section: Introductionmentioning
confidence: 99%
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“…where u(x, t) = (u 1 (x, t), u 2 (x, t), u 3 (x, t)) ∈ R 3 denotes the incompressible velocity field, and p(x, t) ∈ R the hydrostatic pressure; see [1,2,3,4,5,6,7,8,10,11,12,13,18,20,26,28,31] and their references. Here (−∆) α , with α ≥ 1/2, is the fractional Laplacian, see (2.1).…”
Section: Introductionmentioning
confidence: 99%
“…The fractional Laplacian (−∆) α has been studied in many works in the literature (see, for instance, [32,34] and references therein). To cite some models involving this kind of operator, we refer: Diffusion-reaction, Quasi-geostrophic, Cahn-Hilliard, Porous medium, Schrödinger, Ultrasound, Magnetohydrodynamics (MHD), Magnetohydrodynamics-α (MHD-α) and Navier-Stokes itself (see [1,2,3,4,5,6,7,8,9,10,11,12,14,15,16,17,18,21,22,23,24,25,26,27,28,29,30,31,33,35] and references therein). It is important to recall that, by applying the Spectral Theorem, (−∆) α assumes the diagonal form in the Fourier variable, i.e., this is a Fourier multiplier operator with symbol |ξ| 2α (which extends Fourier multiplier property of −∆).…”
Section: Introductionmentioning
confidence: 99%
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