<p>Let <i>f</i>(<i>x</i>) be a smooth strictly convex solution of <Equation ID="Equ45"> <EquationSource Format="TEX">\( \det \left( \tfrac{\partial ^{2}f}{\partial x_{i}\partial x_{j}}\right) =\exp \left\{ \sum _{i=1}^n- a_i\tfrac{\partial f}{\partial x_{i}} +\sum _{i=1}^n b_ix_i+c \right\} \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mo movablelimits="true">det</mo> <mfenced close=")" open="("> <mstyle displaystyle="false" scriptlevel="0"> <mfrac> <mrow> <msup> <mi>∂</mi> <mn>2</mn> </msup> <mi>f</mi> </mrow> <mrow> <mi>∂</mi> <msub> <mi>x</mi> <mi>i</mi> </msub> <mi>∂</mi> <msub> <mi>x</mi> <mi>j</mi> </msub> </mrow> </mfrac> </mstyle> </mfenced> <mo>=</mo> <mo>exp</mo> <mfenced close="}" open="{"> <munderover> <mo>∑</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>n</mi> </munderover> <mo>-</mo> <msub> <mi>a</mi> <mi>i</mi> </msub> <mstyle displaystyle="false" scriptlevel="0"> <mfrac> <mrow> <mi>∂</mi> <mi>f</mi> </mrow> <mrow> <mi>∂</mi> <msub> <mi>x</mi> <mi>i</mi> </msub> </mrow> </mfrac> </mstyle> <mo>+</mo> <munderover> <mo>∑</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>n</mi> </munderover> <msub> <mi>b</mi> <mi>i</mi> </msub> <msub> <mi>x</mi> <mi>i</mi> </msub> <mo>+</mo> <mi>c</mi> </mfenced> </mrow> </math></EquationSource> </Equation>defined on <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {R}^{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(a_i\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>a</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(b_i\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>b</mi> <mi>i</mi> </msub> </math></EquationSource> </InlineEquation> and <i>c</i> are constants. Then, the graph <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(M_{\nabla f}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>M</mi> <mrow> <mi mathvariant="normal">∇</mi> <mi>f</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\nabla f\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">∇</mi> <mi>f</mi> </mrow> </math></EquationSource> </InlineEquation> is a space-like translating soliton for the mean curvature flow in pseudo-Euclidean space <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({\mathbb R}^{2n}_{n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> <mrow> <mn>2</mn> <mi>n</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation> with the indefinite metric <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\sum dx_idy_i\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>∑</mo> <mi>d</mi> <msub> <mi>x</mi> <mi>i</mi> </msub> <mi>d</mi> <msub> <mi>y</mi> <mi>i</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. In this paper, we further investigate the properties of its entire solutions for some special translating vectors <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(T=(a_1,\cdots ,a_n;b_1,\cdots ,b_n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>=</mo> <mo stretchy="false">(</mo> <msub> <mi>a</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi>a</mi> <mi>n</mi> </msub> <mo>;</mo> <msub> <mi>b</mi> <mn>1</mn> </msub> <mo>,</mo> <mo>⋯</mo> <mo>,</mo> <msub> <mi>b</mi> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. In particular, we demonstrate a non-existence result of entire Lagrangian translating soliton on <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {R}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> if <i>T</i> is a lightlike vector with <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\((a_1,a_2)\ne 0,\;(b_1,b_2)\ne 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <msub> <mi>a</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>a</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>≠</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.277778em" /> <mrow> <mo stretchy="false">(</mo> <msub> <mi>b</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>b</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>≠</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and we find that the equation with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(a_1=a_2=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>a</mi> <mn>1</mn> </msub> <mo>=</mo> <msub> <mi>a</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> has a close relation to the Laplacian equation on Euclidean space <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mathbb {R}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>.</p>

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The Entire Solutions for Two-Dimensional Monge-Ampère Equations of Lagrangian Translating Solitons

  • Hongru Song,
  • Yadong Wu,
  • Ruiwei Xu

摘要

Let f(x) be a smooth strictly convex solution of \( \det \left( \tfrac{\partial ^{2}f}{\partial x_{i}\partial x_{j}}\right) =\exp \left\{ \sum _{i=1}^n- a_i\tfrac{\partial f}{\partial x_{i}} +\sum _{i=1}^n b_ix_i+c \right\} \) det 2 f x i x j = exp i = 1 n - a i f x i + i = 1 n b i x i + c defined on \(\mathbb {R}^{n}\) R n , where \(a_i\) a i , \(b_i\) b i and c are constants. Then, the graph \(M_{\nabla f}\) M f of \(\nabla f\) f is a space-like translating soliton for the mean curvature flow in pseudo-Euclidean space \({\mathbb R}^{2n}_{n}\) R n 2 n with the indefinite metric \(\sum dx_idy_i\) d x i d y i . In this paper, we further investigate the properties of its entire solutions for some special translating vectors \(T=(a_1,\cdots ,a_n;b_1,\cdots ,b_n)\) T = ( a 1 , , a n ; b 1 , , b n ) . In particular, we demonstrate a non-existence result of entire Lagrangian translating soliton on \(\mathbb {R}^{2}\) R 2 if T is a lightlike vector with \((a_1,a_2)\ne 0,\;(b_1,b_2)\ne 0\) ( a 1 , a 2 ) 0 , ( b 1 , b 2 ) 0 , and we find that the equation with \(a_1=a_2=0\) a 1 = a 2 = 0 has a close relation to the Laplacian equation on Euclidean space \(\mathbb {R}^3\) R 3 .