<p>We consider a contact Hamiltonian <i>H</i>(<i>x</i>,&#xa0;<i>p</i>,&#xa0;<i>u</i>) with certain dependence on the contact variable <i>u</i>. If <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(u_{-}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation> is a viscosity solution of the contact Hamilton-Jacobi equation <Equation ID="Equ24"> <EquationSource Format="TEX">\(\begin{aligned} H(x,D_{x}u(x),u(x))=0,\quad x\in M, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>H</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <msub> <mi>D</mi> <mi>x</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mi>x</mi> <mo>∈</mo> <mi>M</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(u_{-}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation> is locally asymptotically stable, we prove that the perturbed equation <Equation ID="Equ25"> <EquationSource Format="TEX">\(\begin{aligned} H(x,D_{x}u(x),u(x))+\varepsilon P(x,D_{x}u(x),u(x))=0,\quad x\in M, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mi>H</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <msub> <mi>D</mi> <mi>x</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <mi>ε</mi> <mi>P</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <msub> <mi>D</mi> <mi>x</mi> </msub> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mi>x</mi> <mo>∈</mo> <mi>M</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>has a viscosity solution <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(u_{-}^{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>u</mi> <mrow> <mo>-</mo> </mrow> <mi>ε</mi> </msubsup> </math></EquationSource> </InlineEquation> which converges uniformly to <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(u_{-}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation>, as the perturbation parameter <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation> converges to 0. Moreover, we give a condition ensuring that in a neighborhood of the viscosity solution <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(u_-\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>u</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation>, the perturbed solution <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(u_{-}^{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>u</mi> <mrow> <mo>-</mo> </mrow> <mi>ε</mi> </msubsup> </math></EquationSource> </InlineEquation> is unique. Furthermore, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(u_{-}^{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>u</mi> <mrow> <mo>-</mo> </mrow> <mi>ε</mi> </msubsup> </math></EquationSource> </InlineEquation> is still locally Lyapunov asymptotically stable.</p>

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The existence and stability of viscosity solutions to perturbed contact Hamilton-Jacobi equations

  • Huan Wu,
  • Shiqing Zhang

摘要

We consider a contact Hamiltonian H(xpu) with certain dependence on the contact variable u. If \(u_{-}\) u - is a viscosity solution of the contact Hamilton-Jacobi equation \(\begin{aligned} H(x,D_{x}u(x),u(x))=0,\quad x\in M, \end{aligned}\) H ( x , D x u ( x ) , u ( x ) ) = 0 , x M , and \(u_{-}\) u - is locally asymptotically stable, we prove that the perturbed equation \(\begin{aligned} H(x,D_{x}u(x),u(x))+\varepsilon P(x,D_{x}u(x),u(x))=0,\quad x\in M, \end{aligned}\) H ( x , D x u ( x ) , u ( x ) ) + ε P ( x , D x u ( x ) , u ( x ) ) = 0 , x M , has a viscosity solution \(u_{-}^{\varepsilon }\) u - ε which converges uniformly to \(u_{-}\) u - , as the perturbation parameter \(\varepsilon \) ε converges to 0. Moreover, we give a condition ensuring that in a neighborhood of the viscosity solution \(u_-\) u - , the perturbed solution \(u_{-}^{\varepsilon }\) u - ε is unique. Furthermore, \(u_{-}^{\varepsilon }\) u - ε is still locally Lyapunov asymptotically stable.