Differential and Integral Equations

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Differential and Integral Equations
Volume 38, Numbers 5-6, May/June 2025



To appear in the next issue
Volume 38, Numbers 7-8, July/August 2025


    Ground state solutions for the nonlinear problem involving exponential form of Born-Infeld-like
    Bingbing Dai and Ruifeng Zhang
    Differential and Integral Equations, Volume 38, Number 7/8 (2025), 417-434
    Abstract: In this paper, we investigate dynamical properties in framework of a quasilinear problem in N-dimensional space descended from the Born-Infeld-like nonlinear electromagnetic fields. We establish the existence of the radial ground state solutions of the quasilinear problem involving exponential model based on Born-Infeld theory via dynamical shooting method and some new methods. Our results open up an intriguing perspective for research of other nonlinear systems in Born-Infeld theory including nonlinear arcsin-electromagnetic field, power-law electromagnetic field and so on.


    Asymptotic boundary behavior of large solutions to equations involving infinity Laplacian
    Ling Mi and Yuanda Yue
    Differential and Integral Equations, Volume 38, Number 7/8 (2025), 435-451
    Abstract: The object of this article is to study the asymptotic behavior of the blow-up solutions near the boundary to the following infinity Laplace equation $$ \triangle_{\infty}^{h} u =b(x)f(u), \ x\in \Omega,\ u|_{\partial \Omega}=+\infty, $$ where $$ \triangle_{\infty}^{h}u := |Du|^{h-3}\langle D^{2}uDu, Du \rangle $$ for all $h>1,$ $\Omega$ is a bounded domain with smooth boundary in $\mathbb R^N$, $b \in C(\bar{\Omega})$ which is positive in $\Omega$ and the nonlinearity $f\in C^{1}(0,\infty)$ is positive increasing.


    Existence and asymptotical behavior of solutions for a fractional logarithmic Schrödinger-Poisson system
    Jiaqi Dou, Qi Gao, and Zhengping Wang
    Differential and Integral Equations, Volume 38, Number 7/8 (2025), 453-472
    Abstract: We study the following fractional Schrödinger-Poisson system \begin{equation}\label{eq:0.1} \left\{\begin{array}{ll} (-\Delta)^s u + V(x) u + \lambda\phi (x) u =\mu u+u\log{u^{2}},\ x\in \mathbb{R}^3, \\ (-\Delta)^s\phi = u^2, \displaystyle \ \lim_{|x|\to +\infty}\phi (x)=0, \end{array}\right. \end{equation} where $s\in (\frac{1}{2},1)$, and $\mu,\lambda$ are real parameters. Assuming that $V\in C(\mathbb{R}^3,\mathbb{R}^+)$ and $\lim_{|x|\to +\infty}V(x)=\infty$, we show that problem (\ref{eq:0.1}) has a nonzero solution under suitable assumptions on the parameters $\lambda$ and $\mu$. Moreover, the asymptotical behavior of solutions as $\lambda\to 0$ has also been discussed.


    Poincaré-Perron problem for half-linear ordinary differential equations
    Manabu Naito and Hiroyuki Usami
    Differential and Integral Equations, Volume 38, Number 7/8 (2025), 473-508
    Abstract: This paper deals with the Poincaré-Perron problem for the second order half-linear ordinary differential equation \[ (\Phi_{\alpha}(u'))' + (a_{1} + f_{1}(t)) \Phi_{\alpha}(u') + (a_{2} + f_{2}(t))\Phi_{\alpha}(u) = 0, \] where $\Phi_{\alpha}(u) = |u|^{\alpha}\mathrm{sgn}\, u$ with $\alpha > 0$, and $a_{1}$ and $a_{2}$ are real constants, and $f_{1}(t)$ and $f_{2}(t)$ are real-valued continuous functions on $[t_{0},\infty)$. It is assumed that $\alpha|\lambda|^{\alpha + 1} + a_{1}\Phi_{\alpha}(\lambda) + a_{2} = 0$ has distinct real roots $\lambda_{1}$ and $\lambda_{2}$. Then it is possible to obtain a necessary and sufficient condition for the existence of nonoscillatory solutions $u_{i}(t)$ which satisfy $u_{i}'(t)/u_{i}(t) \to \lambda_{i}$ as $t \to \infty$ ($i = 1, 2$). It is also shown that, in this case, any nontrivial solution $u(t)$ satisfies $u'(t)/u(t) \to \lambda_{1}$ or $\lambda_{2}$ as $t \to \infty$. The classical results for linear equations ($\alpha = 1$) by Hartman-Wintner and the recent results by \v{R}eh\'{a}k, Naito-Usami, Luey-Usami are unified and generalized to the above equation.


    Analyticity in space-time of solutions to evolution equations with multilinear operators based on maximal regularity
    Kei Noda
    Differential and Integral Equations, Volume 38, Number 7/8 (2025), 509-536
    Abstract: Space-time analyticity for evolution equations with nonlinear term represented by multilinear operators is considered via the parameter trick. By extending the case of bilinear operators in the previous work, we obtain space-time analyticity for the equations of Fujita type.


To appear in the next issue
Volume 38, Numbers 9-10, September/October 2025


    Normalized solutions for critical Kirchhoff-Schrödinger-Poisson systems in the Heisenberg group
    Lifeng Guo and Sihua Liang
    Differential and Integral Equations, Volume 38, Number 9/10 (2025), 537-554
    Abstract: In this paper, we consider the existence and multiplicity of normalized solutions for critical Kirchhoff-Possion system involving $p$-sub-Laplacian in the Heisenberg group. Under suitable assumptions, combined with the truncation technique, the concentration-compactness principle, the genus theory, we obtain the existence and multiplicity of the normalized solutions in the $L^p$-subcritical case. To some extent, we extend the results of [19, 30]. Moreover, the result of the paper is completely new in the Euclidean case.


    Scattering for the dispersion managed nonlinear Schrödinger equation
    Mi-Ran Choi, Kiyeon Lee, and Young-Ran Lee
    Differential and Integral Equations, Volume 38, Number 9/10 (2025), 555-576
    Abstract: We consider the dispersion managed nonlinear Schrödinger equations with quintic and cubic nonlinearities in one and two dimensions, respectively. We prove the global well-posedness and scattering in $L_x^2$ for small initial data employing the $U^p$ and $V^p$ spaces.


    The incompressible von Kármán theory for thin pre-strained plates
    Hui Li
    Differential and Integral Equations, Volume 38, Number 9/10 (2025), 577-594
    Abstract: We derive a new version of the von Kármán energy and the corresponding Euler-Lagrange equations, in the context of thin pre-strained plates, under the condition of incompressibility relative to the given pre-strain. Our derivation uses the theory of $\Gamma$-convergence in the calculus of variations, building on prior techniques in [6] and [21].


    On a diffusion equation with rupture
    Yoshikazu Giga and Yuki Ueda
    Differential and Integral Equations, Volume 38, Number 9/10 (2025), 595-618
    Abstract: We propose a model to describe an evolution of a bubble cluster with rupture. In a special case, the equation is reduced to a single parabolic equation with evaporation for the thickness of a liquid layer covering bubbles. If the liquid layer becomes thinner than a given threshold value, we call a rupture occurs. Under assumptions so that the rupture occurs only in a fixed interval of a bubble, we prove that the rupture occurs at infinitely many times and there exists a periodic-in-time solution. Numerical tests indicate that there may not exist a periodic solution if such an assumption is violated.


    On the Strichartz estimate for many body Schrödinger equations on Euclidean cylinder
    Han Wang and Zehua Zhao
    Differential and Integral Equations, Volume 38, Number 9/10 (2025), 619-641
    Abstract: In this short paper, we study the Strichartz estimates for many body Schrödinger equations (MBSE) on Euclidean cylinder (i.e., on semiperiodic space $\mathbb{R}\times \mathbb{T}$, which is also known as a specific type of waveguide manifold), provided that interaction potentials are small enough (depending on the number of the particles and the universal constants, not on the initial data). We will recover the `$L^4_{t,x}$'-type Strichartz estimate as in the standard Schrödinger case (Takaoka-Tzvetkov [35]). This result extends the result of Hong [20] to the Euclidean cylinder case. From another aspect, this also extends [35]'s estimate to the many body case. This result can be also compared with [44] which also studies Strichartz estimates for many body Schrödinger equations on waveguide manifolds. Moreover, we include a well-posedness result for the nonlinear case. At last, we discuss two more related cases: the three-body-interaction case and the fourth-order many body Schrödinger equation case.

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