<p>We prove the existence and regularity of convex solutions to the first initial-boundary value problem for the parabolic Monge–Ampère equation <Equation ID="Equ67"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{aligned} -u_t + \det D^2u&amp;= \psi (x,t) \quad \quad \ \text { in } Q_T,\\ u&amp;=\phi \quad \quad \quad \quad \, \ \text { on } \partial _pQ_T, \end{aligned}\right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <mo>-</mo> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>+</mo> <mo movablelimits="true">det</mo> <msup> <mi>D</mi> <mn>2</mn> </msup> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="1em" /> <mspace width="1em" /> <mspace width="4pt" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <msub> <mi>Q</mi> <mi>T</mi> </msub> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="right"> <mrow> <mrow /> <mi>u</mi> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mo>=</mo> <mi>ϕ</mi> <mspace width="1em" /> <mspace width="1em" /> <mspace width="1em" /> <mspace width="1em" /> <mspace width="0.166667em" /> <mspace width="4pt" /> <mspace width="0.333333em" /> <mtext>on</mtext> <mspace width="0.333333em" /> <msub> <mi>∂</mi> <mi>p</mi> </msub> <msub> <mi>Q</mi> <mi>T</mi> </msub> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\psi ,\phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mo>,</mo> <mi>ϕ</mi> </mrow> </math></EquationSource> </InlineEquation> are given functions, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(Q_T=\Omega \times (0,T]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>Q</mi> <mi>T</mi> </msub> <mo>=</mo> <mi mathvariant="normal">Ω</mi> <mo>×</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mi>T</mi> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\partial _p Q_T\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>∂</mi> <mi>p</mi> </msub> <msub> <mi>Q</mi> <mi>T</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> is the parabolic boundary of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(Q_T\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>Q</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Omega \subset \mathbb {R}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> is a uniformly convex domain. Our approach can also be used to prove similar results for the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-Gauss curvature flow with any <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(0&lt;\gamma \le 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>γ</mi> <mo>≤</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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A priori estimates for parabolic Monge–Ampère type equations

  • Yang Zhou,
  • Ruixuan Zhu

摘要

We prove the existence and regularity of convex solutions to the first initial-boundary value problem for the parabolic Monge–Ampère equation \(\begin{aligned} \left\{ \begin{aligned} -u_t + \det D^2u&= \psi (x,t) \quad \quad \ \text { in } Q_T,\\ u&=\phi \quad \quad \quad \quad \, \ \text { on } \partial _pQ_T, \end{aligned}\right. \end{aligned}\) - u t + det D 2 u = ψ ( x , t ) in Q T , u = ϕ on p Q T , where \(\psi ,\phi \) ψ , ϕ are given functions, \(Q_T=\Omega \times (0,T]\) Q T = Ω × ( 0 , T ] , \(\partial _p Q_T\) p Q T is the parabolic boundary of \(Q_T\) Q T , and \(\Omega \subset \mathbb {R}^n\) Ω R n is a uniformly convex domain. Our approach can also be used to prove similar results for the \(\gamma \) γ -Gauss curvature flow with any \(0<\gamma \le 1\) 0 < γ 1 .