<p>Consider the three-dimensional magnetohydrodynamics (MHD) equations with horizontal dissipation in the upper half-space <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">$\mathbb{R}_{+}^{3}$</EquationSource> </InlineEquation>. First, under appropriate assumptions on the initial velocity and magnetic field in the new-type space <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="fraktur">L</mi> <mi>δ</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>p</mi> </mrow> </msubsup> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathfrak{L}_{\delta}^{p,p}(\mathbb{R}_{+}^{3})$</EquationSource> </InlineEquation>, with the help of the integral equation, we prove the global well-posedness of the system for small initial values. Second, through the linear solution formula and using the space <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="fraktur">L</mi> <mi>δ</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>p</mi> </mrow> </msubsup> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathfrak{L}_{\delta}^{p,p}(\mathbb{R}_{+}^{3})$</EquationSource> </InlineEquation> introduced to overcome the singular integral operators emerging in the solution formula, we obtain the first-order derivatives and the optimal decay rate of the solution in the anisotropic Lebesgue norms. Finally, utilizing the embedding relationship between the <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="fraktur">L</mi> <mrow> <mn>1</mn> </mrow> <mn>1</mn> </msubsup> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$\mathfrak{L}_{1}^{1}(\mathbb{R}_{+}^{3})$</EquationSource> </InlineEquation> space and the <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <msubsup> <mi>L</mi> <mrow> <mn>1</mn> </mrow> <mn>1</mn> </msubsup> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$L_{1}^{1}(\mathbb{R}_{+}^{3})$</EquationSource> </InlineEquation> space, we obtain the uniform <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <msubsup> <mi>L</mi> <mrow> <mn>1</mn> </mrow> <mn>1</mn> </msubsup> <mo stretchy="false">(</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mo>+</mo> <mn>3</mn> </msubsup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">$L_{1}^{1}(\mathbb{R}_{+}^{3})$</EquationSource> </InlineEquation>-estimate of the solution.</p>

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Decay estimates of global solutions for the three-dimensional magnetohydrodynamics equations with horizontal dissipation in a half space

  • Xiao Li

摘要

Consider the three-dimensional magnetohydrodynamics (MHD) equations with horizontal dissipation in the upper half-space R + 3 $\mathbb{R}_{+}^{3}$ . First, under appropriate assumptions on the initial velocity and magnetic field in the new-type space L δ p , p ( R + 3 ) $\mathfrak{L}_{\delta}^{p,p}(\mathbb{R}_{+}^{3})$ , with the help of the integral equation, we prove the global well-posedness of the system for small initial values. Second, through the linear solution formula and using the space L δ p , p ( R + 3 ) $\mathfrak{L}_{\delta}^{p,p}(\mathbb{R}_{+}^{3})$ introduced to overcome the singular integral operators emerging in the solution formula, we obtain the first-order derivatives and the optimal decay rate of the solution in the anisotropic Lebesgue norms. Finally, utilizing the embedding relationship between the L 1 1 ( R + 3 ) $\mathfrak{L}_{1}^{1}(\mathbb{R}_{+}^{3})$ space and the L 1 1 ( R + 3 ) $L_{1}^{1}(\mathbb{R}_{+}^{3})$ space, we obtain the uniform L 1 1 ( R + 3 ) $L_{1}^{1}(\mathbb{R}_{+}^{3})$ -estimate of the solution.