<p>We obtain new quantitative estimates of the vanishing viscosity approximation for time-dependent, degenerate, Hamilton–Jacobi equations that are neither concave nor convex in the gradient and Hessian entries of the form <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\partial _t u+H(x,t,Du,D^2u)=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>u</mi> <mo>+</mo> <mi>H</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <mi>D</mi> <mi>u</mi> <mo>,</mo> <msup> <mi>D</mi> <mn>2</mn> </msup> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> in the whole space. We approximate the PDE with a fully nonlinear, possibly degenerate, elliptic operator <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\varepsilon F(x,t,D^2u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mi>F</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo>,</mo> <msup> <mi>D</mi> <mn>2</mn> </msup> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. Assuming that <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(u\in C^\alpha _x\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>u</mi> <mo>∈</mo> <msubsup> <mi>C</mi> <mi>x</mi> <mi>α</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(u_0\in C^\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>u</mi> <mn>0</mn> </msub> <mo>∈</mo> <msup> <mi>C</mi> <mi>η</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H\in C^\beta _x\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo>∈</mo> <msubsup> <mi>C</mi> <mi>x</mi> <mi>β</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation> and having power growth <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> in the gradient entry, we establish a convergence rate of order <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\varepsilon ^{\min \left\{ \frac{\eta }{2},\frac{\beta +\gamma (\alpha -1)}{\beta +\gamma (\alpha -1)+2-\alpha }\right\} }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mrow> <mo movablelimits="true">min</mo> <mfenced close="}" open="{"> <mfrac> <mi>η</mi> <mn>2</mn> </mfrac> <mo>,</mo> <mfrac> <mrow> <mi>β</mi> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mrow> <mi>β</mi> <mo>+</mo> <mi>γ</mi> <mo stretchy="false">(</mo> <mi>α</mi> <mo>-</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo>+</mo> <mn>2</mn> <mo>-</mo> <mi>α</mi> </mrow> </mfrac> </mfenced> </mrow> </msup> </math></EquationSource> </InlineEquation>. Our novel approach exploits the regularizing properties of sup/inf-convolutions for viscosity solutions and the comparison principle. We also obtain explicit constants and do not assume differentiability properties neither on solutions nor on <i>H</i>. The same method provides new convergence rates for the vanishing viscosity approximation of the stationary counterpart of the equation and for transport equations with Hölder coefficients.</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

Convergence rates for the vanishing viscosity approximation of fully nonlinear, non-convex, second-order Hamilton–Jacobi equations via nonlinear convolutions

  • Alekos Cecchin,
  • Alessandro Goffi

摘要

We obtain new quantitative estimates of the vanishing viscosity approximation for time-dependent, degenerate, Hamilton–Jacobi equations that are neither concave nor convex in the gradient and Hessian entries of the form \(\partial _t u+H(x,t,Du,D^2u)=0\) t u + H ( x , t , D u , D 2 u ) = 0 in the whole space. We approximate the PDE with a fully nonlinear, possibly degenerate, elliptic operator \(\varepsilon F(x,t,D^2u)\) ε F ( x , t , D 2 u ) . Assuming that \(u\in C^\alpha _x\) u C x α , \(u_0\in C^\eta \) u 0 C η , \(H\in C^\beta _x\) H C x β and having power growth \(\gamma \) γ in the gradient entry, we establish a convergence rate of order \(\varepsilon ^{\min \left\{ \frac{\eta }{2},\frac{\beta +\gamma (\alpha -1)}{\beta +\gamma (\alpha -1)+2-\alpha }\right\} }\) ε min η 2 , β + γ ( α - 1 ) β + γ ( α - 1 ) + 2 - α . Our novel approach exploits the regularizing properties of sup/inf-convolutions for viscosity solutions and the comparison principle. We also obtain explicit constants and do not assume differentiability properties neither on solutions nor on H. The same method provides new convergence rates for the vanishing viscosity approximation of the stationary counterpart of the equation and for transport equations with Hölder coefficients.