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On Rayleigh quotients connected to $p$-Laplace equations with polynomial nonlinearities

Vladimir Bobkov, Mieko Tanaka

TL;DR

This work develops a unified variational framework linking $p$-Laplace equations with polynomial nonlinearities to normalized critical points of a $0$-homogeneous Rayleigh-type quotient $R_\alpha(u)$ on $W_0^{1,p}(\Omega)$. By establishing a bijection between solutions of $-\Delta_p u=\mu|u|^{q-2}u+|u|^{r-2}u$ and normalized critical points of $R_\alpha$, the authors obtain a comprehensive spectrum $\lambda_k(\alpha)$ of variational eigenvalues for $\alpha>\alpha_0$, together with detailed analytic properties (bounds, monotonicity, continuity) and the translation level framework $\mu_\alpha$ that connects to the original nonlocal problems. They derive sharp results in subhomogeneous ($q<r\le p$) and superhomogeneous ($p<q<r$) regimes, including simple, isolated ground states and absence of nearby sign-changing critical points, and identify a degenerate, inflection-type family of solutions at $\alpha^*=(r-p)/(r-q)$ in the convex–concave setting. The findings illuminate energy landscapes, multiplicity, and bifurcation behavior for generalized nonlinear eigenvalue problems and offer a robust pathway to classify solutions via the index $k$ of $\lambda_k(\alpha)$. Overall, the work advances a rigorous, parameterized variational approach to nonlocal $p$-Laplacian problems with polynomial nonlinearities and clarifies the interplay between normalization, energy structure, and solution sign patterns.

Abstract

Let $Ω$ be a bounded open set and $p,q,r>1$. The main observation of the present work is the following: $W_0^{1,p}(Ω)$-solutions of the equation $-Δ_p u = μ|u|^{q-2}u + |u|^{r-2}u$ parameterized by $μ$ are in bijection with properly normalized critical points of the $0$-homogeneous Rayleigh type quotient $R_α(u)=\|\nabla u\|_p^p/ (\|u\|_q^{αp} \|u\|_r^{p-αp})$ parameterized by $α$. We study this bijection and properties of $R_α$ for various relations between $p,q,r$. In particular, for the generalized convex-concave problem (the case $q<p<r$) the bijection allows to provide the existence and characterization of all degenerate solutions corresponding to the inflection point of the fibred energy functional: they are critical points of $R_α$ exclusively with $α= (r-p)/(r-q)$. In the subhomogeneous case $q<r \leq p$ and under additional assumptions on $Ω$, the ground state level of $R_α$ is simple and isolated, and minimizers of $R_α$ exhaust the whole set of sign-constant solutions of the corresponding equation. In the superhomogeneous case $p < q<r$, there are no sign-changing critical points in a vicinity of the ground state level of $R_α$.

On Rayleigh quotients connected to $p$-Laplace equations with polynomial nonlinearities

TL;DR

This work develops a unified variational framework linking -Laplace equations with polynomial nonlinearities to normalized critical points of a -homogeneous Rayleigh-type quotient on . By establishing a bijection between solutions of and normalized critical points of , the authors obtain a comprehensive spectrum of variational eigenvalues for , together with detailed analytic properties (bounds, monotonicity, continuity) and the translation level framework that connects to the original nonlocal problems. They derive sharp results in subhomogeneous () and superhomogeneous () regimes, including simple, isolated ground states and absence of nearby sign-changing critical points, and identify a degenerate, inflection-type family of solutions at in the convex–concave setting. The findings illuminate energy landscapes, multiplicity, and bifurcation behavior for generalized nonlinear eigenvalue problems and offer a robust pathway to classify solutions via the index of . Overall, the work advances a rigorous, parameterized variational approach to nonlocal -Laplacian problems with polynomial nonlinearities and clarifies the interplay between normalization, energy structure, and solution sign patterns.

Abstract

Let be a bounded open set and . The main observation of the present work is the following: -solutions of the equation parameterized by are in bijection with properly normalized critical points of the -homogeneous Rayleigh type quotient parameterized by . We study this bijection and properties of for various relations between . In particular, for the generalized convex-concave problem (the case ) the bijection allows to provide the existence and characterization of all degenerate solutions corresponding to the inflection point of the fibred energy functional: they are critical points of exclusively with . In the subhomogeneous case and under additional assumptions on , the ground state level of is simple and isolated, and minimizers of exhaust the whole set of sign-constant solutions of the corresponding equation. In the superhomogeneous case , there are no sign-changing critical points in a vicinity of the ground state level of .

Paper Structure

This paper contains 19 sections, 48 theorems, 163 equations, 5 figures.

Key Result

Lemma 1.1

Let $r \neq p$ and $\mu \in \mathbb{R}$. Let $u \in W_0^{1,p}(\Omega) \setminus \{0\}$ be a solution of either or Then $u$ is a critical point of $R_\alpha$ with $\alpha = \mu \|u\|_q^q/\|\nabla u\|_p^p$, where $\alpha < 1$ in the case of eq:Pconconx, and $\alpha > 1$ in the case of eq:Pconconx2.

Figures (5)

  • Figure 1: Schematically depicted results of Propositions \ref{['prop:omega-to-zero']}--\ref{['prop:boundedness:concon']}, where $\mu_\alpha$ stands for $\underline{\mu}\space_\alpha^k$ or $\overline{\mu}\space_\alpha^k$ for some $k \in \mathbb{N}$.
  • Figure 2: Schematically depicted results of Propositions \ref{['prop:omega-to-zero:u']}--\ref{['prop:omega-to-infty:u']}, where $u_\alpha$ stands for $\underline{u}_\alpha^k$ or $\overline{u}_\alpha^k$ for some $k \in \mathbb{N}$.
  • Figure 3: Schematically depicted bifurcation diagrams for the problems \ref{['eq:Pconconx']}, \ref{['eq:Pconconx2']}, where $\mu_\alpha$ and $u_\alpha$ stand for $\underline{\mu}\space_\alpha^k$ or $\overline{\mu}\space_\alpha^k$, and $\underline{u}_\alpha^k$ or $\overline{u}_\alpha^k$ for some $k \in \mathbb{N}$, respectively.
  • Figure 4: Schematically depicted behavior of $t \mapsto E_{\mu_\alpha}(tu)$ for some $u \in W_0^{1,p}(\Omega) \setminus \{0\}$ and various values of $\mu_\alpha$. A curve with the critical point of inflection type is distinguished.
  • Figure 5: Schematically depicted results of Propositions \ref{['prop:omega:2']}, \ref{['prop:omega:u2']}, where $\nu_\alpha$, $u_\alpha$ stand for $\underline{\nu}_\alpha^k$, $\underline{u}_\alpha^k$ or $\overline{\nu}_\alpha^k$, $\overline{u}_\alpha^k$ for some $k \in \mathbb{N}$.

Theorems & Definitions (99)

  • Lemma 1.1
  • proof
  • Remark 1.2
  • Remark 1.3
  • Lemma 2.1
  • proof
  • Lemma 2.2
  • proof
  • Remark 2.3
  • Remark 2.4
  • ...and 89 more