<p>In this work, we consider the generalized Benjamin-Bona-Mahony equation <Equation ID="Equ146"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_Equ146.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="371" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} \partial _t u+\partial _x u+\partial _x( |u|^pu)-\partial _t \partial _x^{2}u=0, \quad (t,x) \in \mathbb {R} \times \mathbb {R}, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>+</mo> <msub> <mi>∂</mi> <mi>x</mi> </msub> <mi>u</mi> <mo>+</mo> <msub> <mi>∂</mi> <mi>x</mi> </msub> <msup> <mrow> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> <mrow> <mi>u</mi> <mo stretchy="false">)</mo> <mo>-</mo> </mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <msubsup> <mi>∂</mi> <mi>x</mi> <mn>2</mn> </msubsup> <mi>u</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> <mo>×</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>with <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(p&gt;4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&gt;</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>. This equation has the solitary waves solution <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="79" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi _{c}(x-ct), \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ϕ</mi> <mi>c</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>-</mo> <mi>c</mi> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> for any frequency <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq3.gif" Format="GIF" Height="13" Rendition="HTML" Resolution="72" Type="Linedraw" Width="45" /> </InlineMediaObject> <EquationSource Format="TEX">\(c&gt;1.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&gt;</mo> <mn>1</mn> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> It has been proved by Souganidis and Strauss [<CitationRef CitationID="CR10">10</CitationRef>] that, there exists a number <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(c_{0}(p)&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>c</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, such that solitary waves <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi _{c}(x-ct)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ϕ</mi> <mi>c</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>-</mo> <mi>c</mi> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="96" /> </InlineMediaObject> <EquationSource Format="TEX">\(1&lt;c&lt;c_{0}(p) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>c</mi> <mo>&lt;</mo> <msub> <mi>c</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is orbitally unstable, while for <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="71" /> </InlineMediaObject> <EquationSource Format="TEX">\(c&gt;c_{0}(p), \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&gt;</mo> <msub> <mi>c</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(\phi _{c}(x-ct)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ϕ</mi> <mi>c</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>-</mo> <mi>c</mi> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is orbitally stable. The linear exponential instability in the former case was further proved by Pego and Weinstein [<CitationRef CitationID="CR9">9</CitationRef>]. In this paper, we prove the orbital instability in the critical case <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_2981_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(c=c_{0}(p)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>=</mo> <msub> <mi>c</mi> <mn>0</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>p</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Instability of the solitary waves for the generalized Benjamin-Bona-Mahony equation

  • Rui Jia,
  • Yifei Wu

摘要

In this work, we consider the generalized Benjamin-Bona-Mahony equation \(\begin{aligned} \partial _t u+\partial _x u+\partial _x( |u|^pu)-\partial _t \partial _x^{2}u=0, \quad (t,x) \in \mathbb {R} \times \mathbb {R}, \end{aligned}\) t u + x u + x ( | u | p u ) - t x 2 u = 0 , ( t , x ) R × R , with \(p>4\) p > 4 . This equation has the solitary waves solution \(\phi _{c}(x-ct), \) ϕ c ( x - c t ) , for any frequency \(c>1.\) c > 1 . It has been proved by Souganidis and Strauss [10] that, there exists a number \(c_{0}(p)>1\) c 0 ( p ) > 1 , such that solitary waves \(\phi _{c}(x-ct)\) ϕ c ( x - c t ) with \(1<c<c_{0}(p) \) 1 < c < c 0 ( p ) is orbitally unstable, while for \(c>c_{0}(p), \) c > c 0 ( p ) , \(\phi _{c}(x-ct)\) ϕ c ( x - c t ) is orbitally stable. The linear exponential instability in the former case was further proved by Pego and Weinstein [9]. In this paper, we prove the orbital instability in the critical case \(c=c_{0}(p)\) c = c 0 ( p ) .