<p>We investigate the Cauchy problem for the Navier–Stokes equations for viscous compressible fluids with capillarity. The linear third-order capillarity term behaves like the heat diffusion of density fluctuations, which enables us to provide an equivalent characterization of Gevrey analyticity, optimal decay, and initial regularity criteria in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(d \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>). Precisely, in the critical <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation> framework, it is proved that the Besov space <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\dot{B}^{\sigma _1}_{2,\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mover accent="true"> <mi>B</mi> <mo>˙</mo> </mover> <mrow> <mn>2</mn> <mo>,</mo> <mi>∞</mi> </mrow> <msub> <mi>σ</mi> <mn>1</mn> </msub> </msubsup> </math></EquationSource> </InlineEquation>-boundedness condition (with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(d/2-2d/p\le \sigma _1&lt;d/2-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mo>-</mo> <mn>2</mn> <mi>d</mi> <mo stretchy="false">/</mo> <mi>p</mi> <mo>≤</mo> <msub> <mi>σ</mi> <mn>1</mn> </msub> <mo>&lt;</mo> <mi>d</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) of the low-frequency part of initial perturbation is not only sufficient, but also necessary to achieve Gevrey analyticity or upper bounds of decay estimates for arbitrary higher-order derivatives. Furthermore, we show that the upper and lower bounds of decay estimates hold if and only if the low-frequency part of initial perturbation belongs to a nontrivial subset of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\dot{B}^{\sigma _1}_{2,\infty }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mover accent="true"> <mi>B</mi> <mo>˙</mo> </mover> <mrow> <mn>2</mn> <mo>,</mo> <mi>∞</mi> </mrow> <msub> <mi>σ</mi> <mn>1</mn> </msub> </msubsup> </math></EquationSource> </InlineEquation>. Our approach is partly inspired by Hoff-Zumbrun’s spectral analysis, and requires us to establish the uniform bounds on the growth of the radius of analyticity and the faster decay of the discrepancy between the nonlinear solution and the diffusion profile.</p>

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Equivalent characterization on Gevrey analyticity and optimal decay for viscous compressible fluids with capillarity

  • Weixuan Shi,
  • Ling-Yun Shou,
  • Jiang Xu

摘要

We investigate the Cauchy problem for the Navier–Stokes equations for viscous compressible fluids with capillarity. The linear third-order capillarity term behaves like the heat diffusion of density fluctuations, which enables us to provide an equivalent characterization of Gevrey analyticity, optimal decay, and initial regularity criteria in \(\mathbb {R}^d\) R d ( \(d \ge 2\) d 2 ). Precisely, in the critical \(L^p\) L p framework, it is proved that the Besov space \(\dot{B}^{\sigma _1}_{2,\infty }\) B ˙ 2 , σ 1 -boundedness condition (with \(d/2-2d/p\le \sigma _1<d/2-1\) d / 2 - 2 d / p σ 1 < d / 2 - 1 ) of the low-frequency part of initial perturbation is not only sufficient, but also necessary to achieve Gevrey analyticity or upper bounds of decay estimates for arbitrary higher-order derivatives. Furthermore, we show that the upper and lower bounds of decay estimates hold if and only if the low-frequency part of initial perturbation belongs to a nontrivial subset of \(\dot{B}^{\sigma _1}_{2,\infty }\) B ˙ 2 , σ 1 . Our approach is partly inspired by Hoff-Zumbrun’s spectral analysis, and requires us to establish the uniform bounds on the growth of the radius of analyticity and the faster decay of the discrepancy between the nonlinear solution and the diffusion profile.