<p>This paper investigates the existence of energy solutions for a Schrödinger-Maxwell system with a variable exponent on a bounded domain <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {D}\subset \mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">D</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(N\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>), where the <i>p</i>(<i>x</i>)-Laplacian couples the unknown functions <i>u</i> and <i>v</i>. Under the assumptions that <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(f\in L^{m(\cdot )}(\mathcal {D})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <msup> <mi>L</mi> <mrow> <mi>m</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">D</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(m(x)&gt;N/p(x)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mi>N</mi> <mo stretchy="false">/</mo> <mi>p</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and that the continuous exponent satisfies <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(p(\cdot )&gt;1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, a variational approach is employed to establish the existence of weak solutions <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\((u,v)\in \left( W_{0}^{1,p(\cdot )}(\mathcal {D})\right) ^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo>,</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msup> <mfenced close=")" open="("> <msubsup> <mi>W</mi> <mrow> <mn>0</mn> </mrow> <mrow> <mn>1</mn> <mo>,</mo> <mi>p</mi> <mo stretchy="false">(</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">D</mi> <mo stretchy="false">)</mo> </mrow> </mfenced> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> for the considered system. Furthermore, it is shown that this solution is a saddle point of the associated energy functional.</p>

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Existence of weak solutions for variable exponent Schrödinger–Maxwell systems

  • Hichem Khelifi,
  • Mohamed Amine Zouatini

摘要

This paper investigates the existence of energy solutions for a Schrödinger-Maxwell system with a variable exponent on a bounded domain \(\mathcal {D}\subset \mathbb {R}^N\) D R N ( \(N\ge 2\) N 2 ), where the p(x)-Laplacian couples the unknown functions u and v. Under the assumptions that \(f\in L^{m(\cdot )}(\mathcal {D})\) f L m ( · ) ( D ) with \(m(x)>N/p(x)\) m ( x ) > N / p ( x ) and that the continuous exponent satisfies \(p(\cdot )>1\) p ( · ) > 1 , a variational approach is employed to establish the existence of weak solutions \((u,v)\in \left( W_{0}^{1,p(\cdot )}(\mathcal {D})\right) ^2\) ( u , v ) W 0 1 , p ( · ) ( D ) 2 for the considered system. Furthermore, it is shown that this solution is a saddle point of the associated energy functional.