<p>The initial value problem for the incompressible Navier–Stokes system on the whole space <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(n \ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) is considered. The initial datum <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\varvec{a}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">a</mi> </mrow> </math></EquationSource> </InlineEquation> is assumed to be small in the norm of scaling invariant homogeneous Besov spaces <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\dot{B}_{r,\infty }^{-1+n/r}(\mathbb {R}^n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mover accent="true"> <mi>B</mi> <mo>˙</mo> </mover> <mrow> <mi>r</mi> <mo>,</mo> <mi>∞</mi> </mrow> <mrow> <mo>-</mo> <mn>1</mn> <mo>+</mo> <mi>n</mi> <mo stretchy="false">/</mo> <mi>r</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(n&lt;r&lt;\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>&lt;</mo> <mi>r</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We then investigate the decay rates of the scaling invariant norms of the corresponding global solution <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\varvec{u}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">u</mi> </mrow> </math></EquationSource> </InlineEquation> by imposing an additional condition on the low-frequency part of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\varvec{a}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">a</mi> </mrow> </math></EquationSource> </InlineEquation>. In particular, we reveal logarithmic decay rates by changing the condition for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\varvec{a}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">a</mi> </mrow> </math></EquationSource> </InlineEquation> slightly. We show that while the decay rate of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\Vert \varvec{u}(t,\cdot )\Vert _{\dot{B}_{r,\infty }^{-1+n/r}(\mathbb {R}^n)}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mrow> <mo stretchy="false">‖</mo> <mrow> <mi mathvariant="bold-italic">u</mi> </mrow> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msubsup> <mover accent="true"> <mi>B</mi> <mo>˙</mo> </mover> <mrow> <mi>r</mi> <mo>,</mo> <mi>∞</mi> </mrow> <mrow> <mo>-</mo> <mn>1</mn> <mo>+</mo> <mi>n</mi> <mo stretchy="false">/</mo> <mi>r</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> </math></EquationSource> </InlineEquation> improves up to <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(O(t^{-n/r})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <mo stretchy="false">(</mo> <msup> <mi>t</mi> <mrow> <mo>-</mo> <mi>n</mi> <mo stretchy="false">/</mo> <mi>r</mi> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, our decay rates of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\varvec{u}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">u</mi> </mrow> </math></EquationSource> </InlineEquation> are indeed optimal under specific restricted conditions for <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\varvec{a}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">a</mi> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Decay rates of small global solutions to the Navier–Stokes system in scaling invariant homogeneous Besov spaces

  • Taiki Takeuchi

摘要

The initial value problem for the incompressible Navier–Stokes system on the whole space \(\mathbb {R}^n\) R n ( \(n \ge 2\) n 2 ) is considered. The initial datum \(\varvec{a}\) a is assumed to be small in the norm of scaling invariant homogeneous Besov spaces \(\dot{B}_{r,\infty }^{-1+n/r}(\mathbb {R}^n)\) B ˙ r , - 1 + n / r ( R n ) with \(n<r<\infty \) n < r < . We then investigate the decay rates of the scaling invariant norms of the corresponding global solution \(\varvec{u}\) u by imposing an additional condition on the low-frequency part of \(\varvec{a}\) a . In particular, we reveal logarithmic decay rates by changing the condition for \(\varvec{a}\) a slightly. We show that while the decay rate of \(\Vert \varvec{u}(t,\cdot )\Vert _{\dot{B}_{r,\infty }^{-1+n/r}(\mathbb {R}^n)}\) u ( t , · ) B ˙ r , - 1 + n / r ( R n ) improves up to \(O(t^{-n/r})\) O ( t - n / r ) , our decay rates of \(\varvec{u}\) u are indeed optimal under specific restricted conditions for \(\varvec{a}\) a .