<p>Initial value problem (IVP) for the BBM equation posed on the real line <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation> and on the torus <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathbb {T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">T</mi> </math></EquationSource> </InlineEquation> with initial data that are analytic in a strip of width <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(2\sigma _0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <msub> <mi>σ</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> in the complex plane is considered. It is known that the local solution preserves the radius of spatial analyticity during the time of existence; however, this radius may decrease as time evolves. In this work, we study the evolution of the radius of spatial analyticity <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\sigma (t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>σ</mi> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of the solution over time. For the BBM equation posed on the real line <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">R</mi> </math></EquationSource> </InlineEquation>, by introducing appropriate damping terms, we show that the radius of spatial analyticity possesses a fixed positive lower bound uniformly in time. For the BBM equation posed on the periodic domain <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathbb {T}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">T</mi> </math></EquationSource> </InlineEquation>, first we show that the evolution of the radius of spatial analyticity cannot decay faster than <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(ct^{-\frac{2}{3}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <msup> <mi>t</mi> <mrow> <mo>-</mo> <mfrac> <mn>2</mn> <mn>3</mn> </mfrac> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> as the time <i>t</i> goes to infinity, improving the results obtained by Himonas and Petronilho (Proc Am Math Soc 148:2953–2967, 2020). Next, as in the real-line case, in this case too, the evolution of the radius of spatial analyticity is shown to be bounded below by a fixed constant by introducing damping terms.</p>

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Global analytic solution to the IVP for the BBM equation posed on \(\mathbb {R}\) and \(\mathbb {T}\)

  • Mikaela Baldasso,
  • Mahendra Panthee

摘要

Initial value problem (IVP) for the BBM equation posed on the real line \(\mathbb {R}\) R and on the torus \(\mathbb {T}\) T with initial data that are analytic in a strip of width \(2\sigma _0\) 2 σ 0 in the complex plane is considered. It is known that the local solution preserves the radius of spatial analyticity during the time of existence; however, this radius may decrease as time evolves. In this work, we study the evolution of the radius of spatial analyticity \(\sigma (t)\) σ ( t ) of the solution over time. For the BBM equation posed on the real line \(\mathbb {R}\) R , by introducing appropriate damping terms, we show that the radius of spatial analyticity possesses a fixed positive lower bound uniformly in time. For the BBM equation posed on the periodic domain \(\mathbb {T}\) T , first we show that the evolution of the radius of spatial analyticity cannot decay faster than \(ct^{-\frac{2}{3}}\) c t - 2 3 as the time t goes to infinity, improving the results obtained by Himonas and Petronilho (Proc Am Math Soc 148:2953–2967, 2020). Next, as in the real-line case, in this case too, the evolution of the radius of spatial analyticity is shown to be bounded below by a fixed constant by introducing damping terms.