<p>This paper is devoted to the following fractional relativistic Schrödinger equation: <Equation ID="Equ1"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="10255_2024_1031_Article_Equ1.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="330" /> </MediaObject> <EquationSource Format="TEX">\((-\Delta+m^{2})^{s}u+V(x)u=f(x,u),\qquad x\in\mathbb{R}^{N},\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mo stretchy="false">(</mo> <mo>−</mo> <mi mathvariant="normal">Δ</mi> <mo>+</mo> <msup> <mi>m</mi> <mrow> <mn>2</mn> </mrow> </msup> <msup> <mo stretchy="false">)</mo> <mrow> <mi>s</mi> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mi>V</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mi>u</mi> <mo>=</mo> <mi>f</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>u</mi> <mo stretchy="false">)</mo> <mo>,</mo> <mspace width="2em" /> <mi>x</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mrow> <mi>N</mi> </mrow> </msup> <mo>,</mo> </math></EquationSource> </Equation> where (−Δ + <i>m</i><sup>2</sup>)<sup><i>s</i></sup> is the fractional relativistic Schrödinger operator, <i>s</i> ∈ (0, 1), <i>m</i> &gt; 0, <i>V</i>: ℝ<sup><i>N</i></sup> → ℝ is a continuous potential and <i>f</i>: ℝ<sup><i>N</i></sup> × ℝ → ℝ is a superlinear continuous nonlinearity with subcritical growth. We consider the case where the potential <i>V</i> is indefinite so that the relativistic Schrödinger operator (−Δ + <i>m</i><sup>2</sup>)<sup><i>s</i></sup> + <i>V</i> possesses a finite-dimensional negative space. With the help of extension method and Morse theory, the existence of a nontrivial solution for the above problem is obtained.</p>

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Existence of Solutions for a Fractional Relativistic Schrödinger Equation with Indefinite Potentials

  • Jun Wang,
  • Li Wang,
  • Qiao-cheng Zhong

摘要

This paper is devoted to the following fractional relativistic Schrödinger equation: \((-\Delta+m^{2})^{s}u+V(x)u=f(x,u),\qquad x\in\mathbb{R}^{N},\) ( Δ + m 2 ) s u + V ( x ) u = f ( x , u ) , x R N , where (−Δ + m2)s is the fractional relativistic Schrödinger operator, s ∈ (0, 1), m > 0, V: ℝN → ℝ is a continuous potential and f: ℝN × ℝ → ℝ is a superlinear continuous nonlinearity with subcritical growth. We consider the case where the potential V is indefinite so that the relativistic Schrödinger operator (−Δ + m2)s + V possesses a finite-dimensional negative space. With the help of extension method and Morse theory, the existence of a nontrivial solution for the above problem is obtained.