<p>This article studies the norm-inflation phenomena of a periodic initial-value Good Boussinesq equation in low-regularity Sobolev spaces. Particularly, this article demonstrates that the initial-value problem is ill-posed in the periodic Sobolev spaces <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> <mo>-</mo> <mn>2</mn> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for all <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(s&gt;1/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. Our proof is based on a constructive method: we provide smooth initial data that generates solutions with arbitrarily high-norms in <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> <mo>-</mo> <mn>2</mn> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and for arbitrarily short times. The result is sharp in the sense that previous work (Cerpa and Rivas in J Evol Equ 18:1501–1519, 2018; Kishimoto in J Differ Equ 254:2393–2433, 2013) has shown well-posedness for periodic Sobolev indexes of the form <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msubsup> <mi>H</mi> <mi>p</mi> <mrow> <mo>-</mo> <mi>s</mi> <mo>-</mo> <mn>2</mn> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>2</mn> <mi>π</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(s\le 1/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>≤</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Norm-inflation results for the good Boussinesq equation

  • George J. Bautista,
  • Leyter Potenciano-Machado

摘要

This article studies the norm-inflation phenomena of a periodic initial-value Good Boussinesq equation in low-regularity Sobolev spaces. Particularly, this article demonstrates that the initial-value problem is ill-posed in the periodic Sobolev spaces \(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\) H p - s ( 0 , 2 π ) × H p - s - 2 ( 0 , 2 π ) for all \(s>1/2\) s > 1 / 2 . Our proof is based on a constructive method: we provide smooth initial data that generates solutions with arbitrarily high-norms in \(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\) H p - s ( 0 , 2 π ) × H p - s - 2 ( 0 , 2 π ) and for arbitrarily short times. The result is sharp in the sense that previous work (Cerpa and Rivas in J Evol Equ 18:1501–1519, 2018; Kishimoto in J Differ Equ 254:2393–2433, 2013) has shown well-posedness for periodic Sobolev indexes of the form \(H^{-s}_p(0,2 \pi ) \times H^{-s-2}_p(0,2 \pi )\) H p - s ( 0 , 2 π ) × H p - s - 2 ( 0 , 2 π ) with \(s\le 1/2\) s 1 / 2 .