<p>In this paper, we consider the following indefinite fully fractional heat equation involving the master operator <Equation ID="Equ61"> <EquationSource Format="TEX">\(\begin{aligned} (\partial _t -\Delta )^{s} u(x,t) = x_1u^p(x,t)\ \ \text{ in }\ \mathbb {R}^n\times \mathbb {R}, \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </msup> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>x</mi> <mn>1</mn> </msub> <msup> <mi>u</mi> <mi>p</mi> </msup> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mspace width="4pt" /> <mspace width="4pt" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>n</mi> </msup> <mo>×</mo> <mi mathvariant="double-struck">R</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(s\in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(-\infty&lt; p &lt; \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mi>∞</mi> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. Under mild conditions, we prove that there is no positive bounded solutions. To this end, we first show that the solutions are strictly increasing along <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(x_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>x</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> direction by employing the direct method of moving planes. Then by constructing an unbounded sub-solution, we derive the nonexistence of bounded solutions. To circumvent the difficulties caused by the fully fractional master operator, we introduced some new ideas and novel approaches that, as we believe, will become useful tool in studying a variety of other fractional elliptic and parabolic problems.</p>

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Master equations with indefinite nonlinearities

  • Wenxiong Chen,
  • Yahong Guo

摘要

In this paper, we consider the following indefinite fully fractional heat equation involving the master operator \(\begin{aligned} (\partial _t -\Delta )^{s} u(x,t) = x_1u^p(x,t)\ \ \text{ in }\ \mathbb {R}^n\times \mathbb {R}, \end{aligned}\) ( t - Δ ) s u ( x , t ) = x 1 u p ( x , t ) in R n × R , where \(s\in (0,1)\) s ( 0 , 1 ) , and \(-\infty< p < \infty \) - < p < . Under mild conditions, we prove that there is no positive bounded solutions. To this end, we first show that the solutions are strictly increasing along \(x_1\) x 1 direction by employing the direct method of moving planes. Then by constructing an unbounded sub-solution, we derive the nonexistence of bounded solutions. To circumvent the difficulties caused by the fully fractional master operator, we introduced some new ideas and novel approaches that, as we believe, will become useful tool in studying a variety of other fractional elliptic and parabolic problems.