<p>The current paper investigates a class of asymptotically linear Schrödinger equations with the nonlinear term <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(f\in C\left( \mathbb {R},\mathbb {R} \right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <mi>C</mi> <mfenced close=")" open="("> <mi mathvariant="double-struck">R</mi> <mo>,</mo> <mi mathvariant="double-struck">R</mi> </mfenced> </mrow> </math></EquationSource> </InlineEquation> s.t. <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lim \limits _{\left| t\right| \rightarrow \infty }\frac{ f\left( t\right) }{t}=\sigma _0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <munder> <mo movablelimits="false">lim</mo> <mrow> <mfenced close="|" open="|"> <mi>t</mi> </mfenced> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </munder> <mfrac> <mrow> <mi>f</mi> <mfenced close=")" open="("> <mi>t</mi> </mfenced> </mrow> <mi>t</mi> </mfrac> <mo>=</mo> <msub> <mi>σ</mi> <mn>0</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\sigma _0\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>σ</mi> <mn>0</mn> </msub> </math></EquationSource> </InlineEquation> stands for the threshold of essential spectrum of Schrödinger operator. Clearly the Palais-Smale condition fails to hold in this case. Especially under the hypothesis <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\( \left( V_2\right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <msub> <mi>V</mi> <mn>2</mn> </msub> </mfenced> </math></EquationSource> </InlineEquation>, the lack of compactness occurs at the interaction between nonlinear term and continuum spectrum. For this reason, we introduce a bootstrap iteration approach for elliptic equation on <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb {R}^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation>. The iteration is self-contained and can be regarded as a generalization of Agmon-Douglis-Nirenberg theorem (see Agmon et al. (Comm Pure Appl Math 17:35—92, 1964), Agmon et al. (Comm Pure Appl Math 12:623—727, 1959)). The proof characterizes iteration steps independent of the choice of the parameter <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\( \lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>, which are indeed manipulated by intrinsic natures of potentials and nonlinear terms, and furthermore presents precise estimates for asymptotically linear functions or continuous nonlinear terms restricted on a bounded domain <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation> with smooth boundary <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\partial \Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>∂</mi> <mi mathvariant="normal">Ω</mi> </mrow> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {R }^N\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </math></EquationSource> </InlineEquation>. Additionally, a comparison theorem for the spectrum of Schrödinger operator is also established in this paper. With above preparations, we can get a nontrivial solution without mountain pass geometry, and more importantly make an explicit description of nondegeneracy of solutions with monotonicity hypothesis.</p>

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The existence of solutions of Schrödinger equations with essence resonance

  • Chong Li

摘要

The current paper investigates a class of asymptotically linear Schrödinger equations with the nonlinear term \(f\in C\left( \mathbb {R},\mathbb {R} \right) \) f C R , R s.t. \(\lim \limits _{\left| t\right| \rightarrow \infty }\frac{ f\left( t\right) }{t}=\sigma _0\) lim t f t t = σ 0 , where \(\sigma _0\) σ 0 stands for the threshold of essential spectrum of Schrödinger operator. Clearly the Palais-Smale condition fails to hold in this case. Especially under the hypothesis \( \left( V_2\right) \) V 2 , the lack of compactness occurs at the interaction between nonlinear term and continuum spectrum. For this reason, we introduce a bootstrap iteration approach for elliptic equation on \(\mathbb {R}^N\) R N . The iteration is self-contained and can be regarded as a generalization of Agmon-Douglis-Nirenberg theorem (see Agmon et al. (Comm Pure Appl Math 17:35—92, 1964), Agmon et al. (Comm Pure Appl Math 12:623—727, 1959)). The proof characterizes iteration steps independent of the choice of the parameter \( \lambda \) λ , which are indeed manipulated by intrinsic natures of potentials and nonlinear terms, and furthermore presents precise estimates for asymptotically linear functions or continuous nonlinear terms restricted on a bounded domain \(\Omega \) Ω with smooth boundary \(\partial \Omega \) Ω in \(\mathbb {R }^N\) R N . Additionally, a comparison theorem for the spectrum of Schrödinger operator is also established in this paper. With above preparations, we can get a nontrivial solution without mountain pass geometry, and more importantly make an explicit description of nondegeneracy of solutions with monotonicity hypothesis.