Repository of the University of Ljubljana (University of Ljubljana) · 2020 · 60 citations · 37 references
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Natural SciencesMathematicsComputational Fluid DynamicsDifferential EquationsDynamical SystemsPartial Differential EquationsVariational FormulationWeak FormulationCoupled Partial Differential EquationsElliptic Partial Differential EquationsNonlinear Partial Differential EquationsNonlinear Variational ProblemsParabolic Partial Differential EquationsQuasilinear TheoryVariational Methods In Partial Differential EquationsVariational Problems
Abstract This paper deals with the existence of multiple solutions for the quasilinear equation <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mrow><m:mrow><m:mo>-</m:mo><m:mrow><m:mrow><m:mi>div</m:mi><m:mo></m:mo><m:mi>𝐀</m:mi></m:mrow><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mi>x</m:mi><m:mo>,</m:mo><m:mrow><m:mo>∇</m:mo><m:mo></m:mo><m:mi>u</m:mi></m:mrow><m:mo>)</m:mo></m:mrow></m:mrow></m:mrow><m:mo>+</m:mo><m:mrow><m:msup><m:mrow><m:mo>|</m:mo><m:mi>u</m:mi><m:mo>|</m:mo></m:mrow><m:mrow><m:mrow><m:mi>α</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mi>x</m:mi><m:mo>)</m:mo></m:mrow></m:mrow><m:mo>-</m:mo><m:mn>2</m:mn></m:mrow></m:msup><m:mo></m:mo><m:mi>u</m:mi></m:mrow></m:mrow><m:mo>=</m:mo><m:mrow><m:mrow><m:mi>f</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mi>x</m:mi><m:mo>,</m:mo><m:mi>u</m:mi><m:mo>)</m:mo></m:mrow></m:mrow><m:mo> </m:mo><m:mrow><m:mtext>in </m:mtext><m:msup><m:mi>ℝ</m:mi><m:mi>N</m:mi></m:msup><m:mtext>,</m:mtext></m:mrow></m:mrow></m:mrow></m:math> {-\operatorname{div}\mathbf{A}(x,\nabla u)+|u|^{\alpha(x)-2}u=f(x,u)\quad\text% {in ${\mathbb{R}^{N}}$,}} which involves a general variable exponent elliptic operator <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mi>𝐀</m:mi></m:math> {\mathbf{A}} in divergence form. The problem corresponds to double phase anisotropic phenomena, in the sense that the differential operator has various types of behavior like <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:msup><m:mrow><m:mo>|</m:mo><m:mi>ξ</m:mi><m:mo>|</m:mo></m:mrow><m:mrow><m:mrow><m:mi>q</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mi>x</m:mi><m:mo>)</m:mo></m:mrow></m:mrow><m:mo>-</m:mo><m:mn>2</m:mn></m:mrow></m:msup><m:mo></m:mo><m:mi>ξ</m:mi></m:mrow></m:math> {|\xi|^{q(x)-2}\xi} for small <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mo>|</m:mo><m:mi>ξ</m:mi><m:mo>|</m:mo></m:mrow></m:math> {|\xi|} and like <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:msup><m:mrow><m:mo>|</m:mo><m:mi>ξ</m:mi><m:mo>|</m:mo></m:mrow><m:mrow><m:mrow><m:mi>p</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mi>x</m:mi><m:mo>)</m:mo></m:mrow></m:mrow><m:mo>-</m:mo><m:mn>2</m:mn></m:mrow></m:msup><m:mo></m:mo><m:mi>ξ</m:mi></m:mrow></m:math> {|\xi|^{p(x)-2}\xi} for large <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mo>|</m:mo><m:mi>ξ</m:mi><m:mo>|</m:mo></m:mrow></m:math> {|\xi|} , where <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mn>1</m:mn><m:mo><</m:mo><m:mrow><m:mi>α</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mo>⋅</m:mo><m:mo>)</m:mo></m:mrow></m:mrow><m:mo>≤</m:mo><m:mrow><m:mi>p</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mo>⋅</m:mo><m:mo>)</m:mo></m:mrow></m:mrow><m:mo><</m:mo><m:mrow><m:mi>q</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mo>⋅</m:mo><m:mo>)</m:mo></m:mrow></m:mrow><m:mo><</m:mo><m:mi>N</m:mi></m:mrow></m:math> {1<\alpha(\,\cdot\,)\leq p(\,\cdot\,)<q(\,\cdot\,)<N} . Our aim is to approach variationally the problem by using the tools of critical points theory in generalized Orlicz–Sobolev spaces with variable exponent. Our results extend the previous works [A. Azzollini, P. d’Avenia and A. Pomponio, Quasilinear elliptic equations in <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:msup><m:mi>ℝ</m:mi><m:mi>N</m:mi></m:msup></m:math> \mathbb{R}^{N} via variational methods and Orlicz–Sobolev embeddings, Calc. Var. Partial Differential Equations 49 2014, 1–2, 197–213] and [N. Chorfi and V. D. Rădulescu, Standing wave solutions of a quasilinear degenerate Schrödinger equation with unbounded potential, Electron. J. Qual. Theory Differ. Equ. 2016 2016, Paper No. 37] from cases where the exponents p and q are constant, to the case where <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mi>p</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mo>⋅</m:mo><m:mo>)</m:mo></m:mrow></m:mrow></m:math> {p(\,\cdot\,)} and <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mrow><m:mi>q</m:mi><m:mo></m:mo><m:mrow><m:mo>(</m:mo><m:mo>⋅</m:mo><m:mo>)</m:mo></m:mrow></m:mrow></m:math> {q(\,\cdot\,)} are functions. We also substantially weaken some of the hypotheses in these papers and we overcome the lack of compactness by using the weighting method.
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