<p>The global well-posedness of the damped Benjamin-Bona-Mahony equation is investigated in the <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(L^{p}\)</EquationSource> </InlineEquation>-based Sobolev space class <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\dot{H}^{s,p}({\mathbb {T}}^{3}).\)</EquationSource> </InlineEquation> Firstly, using bilinear estimates and contraction mapping principle, the local well-posedness of the equation is originally shown in <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\dot{H}^{s,p}({\mathbb {T}}^{3})\)</EquationSource> </InlineEquation> with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(s \ge \max \{0,\frac{3}{p}-1\}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\frac{3}{2}\le p&lt;\infty .\)</EquationSource> </InlineEquation> Secondly, using high-low frequency decomposition and Sobolev embedding, the global well-posedness of the damped Benjamin–Bona–Mahony is furthermore studied in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\dot{H}^{s,p}({\mathbb {T}}^{3})\)</EquationSource> </InlineEquation> with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\( \max \{0,\frac{3}{p}-1\}\le s\le 1\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\frac{3}{2}\le p\le 2\)</EquationSource> </InlineEquation>.</p>

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Global Well-Posedness for the 3D Damped Benjamin–Bona–Mahony Equation in \(L^{p}\) Based Sobolev Space

  • Jialong Chen,
  • Yanfeng Guo,
  • Xinglong Wu,
  • Shaokang Yang

摘要

The global well-posedness of the damped Benjamin-Bona-Mahony equation is investigated in the \(L^{p}\) -based Sobolev space class \(\dot{H}^{s,p}({\mathbb {T}}^{3}).\) Firstly, using bilinear estimates and contraction mapping principle, the local well-posedness of the equation is originally shown in \(\dot{H}^{s,p}({\mathbb {T}}^{3})\) with \(s \ge \max \{0,\frac{3}{p}-1\}\) and \(\frac{3}{2}\le p<\infty .\) Secondly, using high-low frequency decomposition and Sobolev embedding, the global well-posedness of the damped Benjamin–Bona–Mahony is furthermore studied in \(\dot{H}^{s,p}({\mathbb {T}}^{3})\) with \( \max \{0,\frac{3}{p}-1\}\le s\le 1\) and \(\frac{3}{2}\le p\le 2\) .