<p>In this paper, a tempered mixed fractional <i>p</i>-Laplacian equation is considered in different regions. By introducing a tempered mixed fractional <i>p</i>-Laplacian operator, we first establish <i>Narrow region principle</i>, which plays a crucial role in the later process. Then we obtain radial symmetry and nonexistence results by using the direct method of moving planes under the circumstance of <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {B}_{1}^{n}(0)\times \mathbb {B}_{1}^{m}(0)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="double-struck">B</mi> <mrow> <mn>1</mn> </mrow> <mi>n</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>×</mo> <msubsup> <mi mathvariant="double-struck">B</mi> <mrow> <mn>1</mn> </mrow> <mi>m</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {R}_{+}^{n}\times \mathbb {R}_{+}^{m}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="double-struck">R</mi> <mrow> <mo>+</mo> </mrow> <mi>n</mi> </msubsup> <mo>×</mo> <msubsup> <mi mathvariant="double-struck">R</mi> <mrow> <mo>+</mo> </mrow> <mi>m</mi> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, respectively.</p>

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Radial symmetry and nonexistence of positive solution for tempered mixed fractional p-Laplacian equations

  • Wenwen Hou,
  • Lihong Zhang

摘要

In this paper, a tempered mixed fractional p-Laplacian equation is considered in different regions. By introducing a tempered mixed fractional p-Laplacian operator, we first establish Narrow region principle, which plays a crucial role in the later process. Then we obtain radial symmetry and nonexistence results by using the direct method of moving planes under the circumstance of \(\mathbb {B}_{1}^{n}(0)\times \mathbb {B}_{1}^{m}(0)\) B 1 n ( 0 ) × B 1 m ( 0 ) and \(\mathbb {R}_{+}^{n}\times \mathbb {R}_{+}^{m}\) R + n × R + m , respectively.