<p>Consider the following Hénon type system: <Equation ID="Equ1"> <EquationNumber>0.1</EquationNumber> <EquationSource Format="TEX">\(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u = |x|^{\alpha } v^{p},\;\;\; &amp; \text {in } \;\; B_1(0),\\ -\Delta v = |x|^{\alpha } u^{q},\;\;\; &amp; \text {in }\;\; B_1(0),\\ u = v= 0, &amp; \text {on } \partial B_1(0), \end{array}\right. } \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>α</mi> </msup> <msup> <mi>v</mi> <mi>p</mi> </msup> <mo>,</mo> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <mspace width="0.277778em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>x</mi> <mo stretchy="false">|</mo> </mrow> <mi>α</mi> </msup> <msup> <mi>u</mi> <mi>q</mi> </msup> <mo>,</mo> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <mspace width="0.277778em" /> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="0.277778em" /> <mspace width="0.277778em" /> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mi>u</mi> <mo>=</mo> <mi>v</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> </mrow> </mtd> <mtd columnalign="left"> <mrow> <mtext>on</mtext> <mspace width="0.333333em" /> <mi>∂</mi> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(B_1(0)\subset \mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>B</mi> <mn>1</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> is the unit ball centered at the origin, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha &gt; 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(p, q&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> satisfy: <Equation ID="Equ2"> <EquationSource Format="TEX">\( \dfrac{1}{p+1} + \dfrac{1}{q+1} &gt; \dfrac{N-2}{N}. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mn>1</mn> <mrow> <mi>p</mi> <mo>+</mo> <mn>1</mn> </mrow> </mfrac> </mstyle> <mo>+</mo> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mn>1</mn> <mrow> <mi>q</mi> <mo>+</mo> <mn>1</mn> </mrow> </mfrac> </mstyle> <mo>&gt;</mo> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> <mi>N</mi> </mfrac> </mstyle> <mo>.</mo> </mrow> </math></EquationSource> </Equation>It is shown that the ground state solution of Eq. <InternalRef RefID="Equ1">0.1</InternalRef> exists for each <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and satisfies the foliated Schwartz symmetry property when <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> is large. In this paper, we first investigate the asymptotic behavior of the ground state solution <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\( ( u_\alpha , v_\alpha )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mi>u</mi> <mi>α</mi> </msub> <mo>,</mo> <msub> <mi>v</mi> <mi>α</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for Eq. <InternalRef RefID="Equ1">0.1</InternalRef>, as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\alpha \rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. Then we analyse the profile of the solutions with one peak or multiple peaks.</p>

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Asymptotic Behavior of Ground State Solution to Hénon type System

  • Yuxia Guo,
  • Congzheng Xuanyuan,
  • Tingfeng Yuan

摘要

Consider the following Hénon type system: 0.1 \(\begin{aligned} {\left\{ \begin{array}{ll} -\Delta u = |x|^{\alpha } v^{p},\;\;\; & \text {in } \;\; B_1(0),\\ -\Delta v = |x|^{\alpha } u^{q},\;\;\; & \text {in }\;\; B_1(0),\\ u = v= 0, & \text {on } \partial B_1(0), \end{array}\right. } \end{aligned}\) - Δ u = | x | α v p , in B 1 ( 0 ) , - Δ v = | x | α u q , in B 1 ( 0 ) , u = v = 0 , on B 1 ( 0 ) , where \(B_1(0)\subset \mathbb {R}^N\) B 1 ( 0 ) R N is the unit ball centered at the origin, \(N\ge 3\) N 3 , \(\alpha > 0\) α > 0 and \(p, q>1\) p , q > 1 satisfy: \( \dfrac{1}{p+1} + \dfrac{1}{q+1} > \dfrac{N-2}{N}. \) 1 p + 1 + 1 q + 1 > N - 2 N . It is shown that the ground state solution of Eq. 0.1 exists for each \(\alpha >0\) α > 0 and satisfies the foliated Schwartz symmetry property when \(\alpha \) α is large. In this paper, we first investigate the asymptotic behavior of the ground state solution \( ( u_\alpha , v_\alpha )\) ( u α , v α ) for Eq. 0.1, as \(\alpha \rightarrow +\infty \) α + . Then we analyse the profile of the solutions with one peak or multiple peaks.