<p>We are interested in the nonlinear damped Klein–Gordon equation <Equation ID="Equ129"> <EquationSource Format="TEX">\( \partial _t^2 u+2\alpha \partial _t u-\Delta u+u-|u|^{p-1}u=0 \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msubsup> <mi>∂</mi> <mi>t</mi> <mn>2</mn> </msubsup> <mi>u</mi> <mo>+</mo> <mn>2</mn> <mi>α</mi> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>+</mo> <mi>u</mi> <mo>-</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> <mi>u</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </Equation>on <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(2\leqslant d\leqslant 5\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>⩽</mo> <mi>d</mi> <mo>⩽</mo> <mn>5</mn> </mrow> </math></EquationSource> </InlineEquation> and energy sub-critical exponents <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(2&lt; p &lt; \frac{d+2}{d-2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mfrac> <mrow> <mi>d</mi> <mo>+</mo> <mn>2</mn> </mrow> <mrow> <mi>d</mi> <mo>-</mo> <mn>2</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. We construct multi-soliton, that is, solutions which behave for large times as a sum of decoupled solitons, in various configurations with symmetry: this includes multi-soliton whose soliton centers lie at the vertices of an expanding regular polygon (with or without a center), of a regular polyhedron (with a center), of a higher dimensional regular polytope, or on a line. We give a precise description of these multi-solitons, in particular the interaction between nearest neighbour solitons is asymptotic to <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\ln t - \frac{d-1}{2} \ln \ln t\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>ln</mo> <mi>t</mi> <mo>-</mo> <mfrac> <mrow> <mi>d</mi> <mo>-</mo> <mn>1</mn> </mrow> <mn>2</mn> </mfrac> <mo>ln</mo> <mo>ln</mo> <mi>t</mi> </mrow> </math></EquationSource> </InlineEquation> as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(t \rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>t</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. We also prove that in any multi-soliton, the solitons cannot share all the same sign. Both statements generalize and refine the results of [13,14] and are based on the analysis developed in [8,9].</p>

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Construction of multi solitary waves with symmetry for the nonlinear damped Klein–Gordon equation

  • Raphaël Côte,
  • Haiming Du

摘要

We are interested in the nonlinear damped Klein–Gordon equation \( \partial _t^2 u+2\alpha \partial _t u-\Delta u+u-|u|^{p-1}u=0 \) t 2 u + 2 α t u - Δ u + u - | u | p - 1 u = 0 on \(\mathbb {R}^d\) R d for \(2\leqslant d\leqslant 5\) 2 d 5 and energy sub-critical exponents \(2< p < \frac{d+2}{d-2}\) 2 < p < d + 2 d - 2 . We construct multi-soliton, that is, solutions which behave for large times as a sum of decoupled solitons, in various configurations with symmetry: this includes multi-soliton whose soliton centers lie at the vertices of an expanding regular polygon (with or without a center), of a regular polyhedron (with a center), of a higher dimensional regular polytope, or on a line. We give a precise description of these multi-solitons, in particular the interaction between nearest neighbour solitons is asymptotic to \(\ln t - \frac{d-1}{2} \ln \ln t\) ln t - d - 1 2 ln ln t as \(t \rightarrow +\infty \) t + . We also prove that in any multi-soliton, the solitons cannot share all the same sign. Both statements generalize and refine the results of [13,14] and are based on the analysis developed in [8,9].