Maximum w-cyclic holey group divisible packings and their application to three-dimensional optical orthogonal codes

Motivated by the application to three-dimensional optical orthogonal codes, we consider the construction for a w-cyclic holey group divisible packing of type $(u,w^v)$ with block size three (3-HGDP for short). A maximum w-cyclic 3-HGDP of type $(u,w^v)$ contains the largest possible number of base blocks. When $u\equiv 0,1(\mathrm{mod}3)$, the exact size of maximum w-cyclic 3-HGDP of type $(u,w^v)$ has been determined in our previous work. Based on recursive constructions, in this paper we establish a framework to construct maximum w-cyclic 3-HGDPs of type $(u,w^v)$ where $u\equiv 2$ (mod 3). In the process, direct constructions on several key auxiliary designs are displayed by choosing appropriate automorphism groups. Eventually, the sizes of maximum w-cyclic 3-HGDPs of type $(u,w^v)$ are determined for all positive integers $u,v$ and w, only leaving a small fraction of possible exceptions unresolved. Furthermore, application of our results to three-dimensional optical orthogonal codes is presented.     

Blow-up phenomena for the Liouville equation with a singular source of integer multiplicity

We are concerned with the existence of blowing-up solutions to the following boundary value problem

$?\mathrm{\Delta }u=\lambda a(x)e^u?4\pi N{\delta }_0\text{ in }\mathrm{\Omega },u=0\text{ on }?\mathrm{\Omega },$

where Ω is a smooth and bounded domain in ${\mathbb{R}}^2$ such that $0\in \mathrm{\Omega }$, $a(x)$ is a positive smooth function, N is a positive integer and $\lambda >0$ is a small parameter. Here ${\delta }_0$ defines the Dirac measure with pole at 0. We find conditions on the function a and on the domain Ω under which there exists a solution $u_{\lambda }$ blowing up at 0 and satisfying $\lambda {\int }_{\mathrm{\Omega }}a(x)e^{u_{\lambda }}\to 8\pi (N+1)$ as $\lambda \to 0^{+}$.     

Existence and nonexistence of positive solutions for a static Schrödinger–Poisson–Slater equation

In this paper we study the following type of the Schrödinger–Poisson–Slater equation with critical growth

$?△u+(u^2?\frac{1}{|4\pi x|})u=\mu |u{|}^{p?1}u+|u{|}^{4}u,\text{in}{\mathbb{R}}^3,$

where $\mu >0$ and $p\in (11/7,5)$. For the case of $p\in (2,5)$. We develop a novel perturbation approach, together with the well-known Mountion–Pass theorem, to prove the existence of positive ground states. For the case of $p=2$, we obtain the nonexistence of nontrivial solutions by restricting the range of μ and also study the existence of positive solutions by the constrained minimization method. For the case of $p\in (11/7,2)$, we use a truncation technique developed by Brezis and Oswald [9] together with a measure representation concentration-compactness principle due to Lions [27] to prove the existence of radial symmetrical positive solutions for $\mu \in (0,{\mu }^{?})$ with some ${\mu }^{?}>0$. The above results nontrivially extend some theorems on the subcritical case obtained by Ianni and Ruiz [18] to the critical case.     

Exact decay estimate on solutions of critical p-Laplacian equations in R+N

Consider the critical p-Laplacian equation in ${\mathbb{R}}_{+}^N$

$\{\begin{array}{cc}\hfill & ?{\mathrm{\Delta }}_{p}u=0,\text{in}{\mathbb{R}}_{+}^N,\hfill \\ \hfill & |\mathrm{?}u{|}^{p?2}\frac{?u}{?n}=|u{|}^{\stackrel{￣}{p}?2}u,\text{on}{\mathbb{R}}^{N?1},\hfill \end{array}$

where ${\mathbb{R}}_{+}^N={\mathbb{R}}^{N?1}\times (0,\infty )$, $1<p<N,\stackrel{￣}{p}=\frac{(N?1)p}{N?p}$ is the critical exponent of the Sobolev imbedding from $W^{1,p}({\mathbb{R}}_{+}^N)$ to $L^q({\mathbb{R}}^{N?1})$, $p\le q\le \stackrel{￣}{p}$ and ${\mathrm{\Delta }}_p$ is the p-Laplacian operator, ${\mathrm{\Delta }}_{p}u=\mathrm{?}(|\mathrm{?}u{|}^{p?2}\mathrm{?}u)$. We prove polynomial decay of the solutions

$|u(x)|\le c{(1+|x|)}^{?\frac{N?p}{p?1}},\text{for}x\in {\mathbb{R}}_{+}^N.$

The decay exponent is the best possible.     

Phase transition layers with boundary intersection for an inhomogeneous Allen–Cahn equation

We consider the nonlinear problem of inhomogeneous Allen–Cahn equation

${?}^2\mathrm{\Delta }u+V(y)u(1?u^2)=0\text{in}\mathrm{\Omega },\frac{?u}{?\nu }=0\text{on}?\mathrm{\Omega },$

where Ω is a bounded domain in ${\mathbb{R}}^2$ with smooth boundary, ? is a small positive parameter, ν denotes the unit outward normal of ?Ω, V is a positive smooth function on $\overline{\mathrm{\Omega }}$. Let Γ be a curve intersecting orthogonally with ?Ω at exactly two points and dividing Ω into two parts. Moreover, Γ satisfies stationary and non-degenerate conditions with respect to the functional ${\int }_{\mathrm{\Gamma }}{V}^{1/2}$. We can prove that there exists a solution $u_{?}$ such that: as $?\to 0$, $u_{?}$ approaches +1 in one part of Ω, while tends to ?1 in the other part, except a small neighborhood of Γ.     

Blowup of solutions to a two-chemical substances chemotaxis system in the critical dimension

This paper deals with positive solutions of the fully parabolic system

$\{\begin{array}{cc}{u}_t=\mathrm{\Delta }u?\chi \mathrm{?}?(u\mathrm{?}v)\hfill & \mathrm{in}\mathrm{\Omega }\times (0,\infty ),\hfill \\ {\tau }_1{v}_t=\mathrm{\Delta }v?v+w\hfill & \mathrm{in}\mathrm{\Omega }\times (0,\infty ),\hfill \\ {\tau }_2{w}_t=\mathrm{\Delta }w?w+u\hfill & \mathrm{in}\mathrm{\Omega }\times (0,\infty )\hfill \end{array}$

under mixed boundary conditions (no-flux and Dirichlet conditions) in a smooth bounded convex domain $\mathrm{\Omega }?{\mathbb{R}}^4$ with positive parameters ${\tau }_1,{\tau }_2,\chi >0$ and nonnegative smooth initial data $(u_0,v_0,w_0)$.Global existence and boundedness of solutions were shown if ${6u_{0}6}_{L^1(\mathrm{\Omega })}<{(8\pi )}^2/\chi$ in Fujie–Senba (2017). In the present paper, it is shown that there exist blowup solutions satisfying ${6u_{0}6}_{L^1(\mathrm{\Omega })}>{(8\pi )}^2/\chi$. This result suggests that the system can be regard as a generalization of the Keller–Segel system, which has $8\pi /\chi$-dichotomy. The key ingredients are a Lyapunov functional and quantization properties of stationary solutions of the system in ${\mathbb{R}}^4$.     

On the existence of weak solutions of semilinear elliptic equations and systems with Hardy potentials

Let $\mathrm{\Omega }?{\mathbb{R}}^N$ ($N\ge 3$) be a bounded $C^2$ domain and $\delta (x)=\mathrm{dist}(x,?\mathrm{\Omega })$. Put $L_{\mu }=\mathrm{\Delta }+\frac{\mu }{{\delta }^2}$ with $\mu >0$. In this paper, we provide various necessary and sufficient conditions for the existence of weak solutions to

$?L_{\mu }u=u^p+\tau \text{in }\mathrm{\Omega },u=\nu \text{on }?\mathrm{\Omega },$

where $\mu >0$, $p>0$, τ and ν are measures on Ω and ?Ω respectively. We then establish existence results for the system

$\{\begin{array}{cc}\hfill & ?L_{\mu }u=?v^p+\tau \text{in }\mathrm{\Omega },\hfill \\ \hfill & ?L_{\mu }v=?u^{\stackrel{?}{p}}+\stackrel{?}{\tau }\text{in }\mathrm{\Omega },\hfill \\ \hfill & u=\nu ,v=\stackrel{?}{\nu }\text{on }?\mathrm{\Omega },\hfill \end{array}$

where $?=\pm 1$, $p>0$, $\stackrel{?}{p}>0$, τ and $\stackrel{?}{\tau }$ are measures on Ω, ν and $\stackrel{?}{\nu }$ are measures on ?Ω. We also deal with elliptic systems where the nonlinearities are more general.     

A three-dimensional Keller–Segel–Navier–Stokes system with logistic source: Global weak solutions and asymptotic stabilization

The Keller–Segel–Navier–Stokes system

(?)$\{\begin{array}{ccc}\hfill n_t+u?\mathrm{?}n& \hfill =\hfill & \mathrm{\Delta }n?\chi \mathrm{?}?(n\mathrm{?}c)+\rho n?\mu n^2,\hfill \\ \hfill c_t+u?\mathrm{?}c& \hfill =\hfill & \mathrm{\Delta }c?c+n,\hfill \\ \hfill u_t+(u?\mathrm{?})u& \hfill =\hfill & \mathrm{\Delta }u+\mathrm{?}P+n\mathrm{?}?+f(x,t),\hfill \\ \hfill \mathrm{?}?u& \hfill =\hfill & 0,\hfill \end{array}$

is considered in a bounded convex domain $\mathrm{\Omega }?{\mathbb{R}}^3$ with smooth boundary, where $?\in W^{1,\infty }(\mathrm{\Omega })$ and $f\in C^1(\overline{\mathrm{\Omega }}\times [0,\infty ))$, and where $\chi >0,\rho \in \mathbb{R}$ and $\mu >0$ are given parameters.It is proved that under the assumption that ${\sup }_{t>0}?{\int }_t^{t+1}{6f(?,s)6}_{L^{\frac{6}{5}}(\mathrm{\Omega })}ds$ be finite, for any sufficiently regular initial data $(n_0,c_0,u_0)$ satisfying $n_0\ge 0$ and $c_0\ge 0$, the initial-value problem for (?) under no-flux boundary conditions for n and c and homogeneous Dirichlet boundary conditions for u possesses at least one globally defined solution in an appropriate generalized sense, and that this solution is uniformly bounded in with respect to the norm in $L^1(\mathrm{\Omega })\times L^6(\mathrm{\Omega })\times L^2(\mathrm{\Omega };{\mathbb{R}}^3)$.Moreover, under the explicit hypothesis that $\mu >\frac{\chi \sqrt{{\rho }_{+}}}{4}$, these solutions are shown to stabilize toward a spatially homogeneous state in their first two components by satisfying

$\begin{array}{c}(n(?,t),c(?,t))\to (\frac{{\rho }_{+}}{\mu },\frac{{\rho }_{+}}{\mu })\text{in }{L}^1(\mathrm{\Omega })\times L^p(\mathrm{\Omega })\hfill \\ \text{for all }p\in [1,6)\text{as }t\to \infty .\hfill \end{array}$

Finally, under an additional condition on temporal decay of f it is shown that also the third solution component equilibrates in that $u(?,t)\to 0$ in $L^2(\mathrm{\Omega };{\mathbb{R}}^3)$ as $t\to \infty$.     

Positive solutions for a class of singular quasilinear Schrödinger equations with critical Sobolev exponent

We prove the existence of positive solutions of the following singular quasilinear Schrödinger equations at critical growth

$?\mathrm{\Delta }u?\lambda c(x)u?\kappa \alpha (\mathrm{\Delta }(|u{|}^{2\alpha }))|u{|}^{2\alpha ?2}u=|u{|}^{q?2}u+|u{|}^{2^{?}?2}u,u\in D^{1,2}({\mathbb{R}}^N),$

via variational methods, where $\lambda \ge 0$, $c:{\mathbb{R}}^N\to {\mathbb{R}}^{+}$, $\kappa >0$, $0<\alpha <1/2$, $2<q<2^{?}$. It is interesting that we do not need to add a weight function to control $|u{|}^{q?2}u$.     

Lorentz estimates for a class of nonlinear parabolic systems

In this paper we obtain the following local Lorentz estimates

$B\left(\left|F\right|\right)\in L_{loc}^{\gamma ,q}?B\left(\left|\mathrm{?}u\right|\right)\in L_{loc}^{\gamma ,q}\text{for any}\gamma >1\text{and}0<q\le \infty$

of the weak solutions for a class of quasilinear parabolic systems

$u_t?\text{div}\left(a\left(\left|\mathrm{?}u\right|\right)\mathrm{?}u\right)=\text{div}\left(a\left(\left|F\right|\right)F\right),$

where $B(t)={\int }_0^t\tau a(\tau )d\tau$ for $t\ge 0$.     

Existence of nontrivial solutions for modified nonlinear fourth-order elliptic equations with indefinite potential

In this paper, we investigate the following modified nonlinear fourth-order elliptic equations$\{\begin{array}{cc}{\mathrm{\Delta }}^{2}u?\mathrm{\Delta }u+V(x)u?\frac{1}{2}u\mathrm{\Delta }(u^2)=g(u),\hfill & \text{in}{\mathbb{R}}^N,\hfill \\ u\in H^2({\mathbb{R}}^N)\hfill \end{array}$ where ${\mathrm{\Delta }}^2=\mathrm{\Delta }(\mathrm{\Delta })$ is the biharmonic operator, V is an indefinite potential, g grows subcritically and satisfies the Ambrosetti-Rabinowitz type condition $g(t)t\ge \mu G(t)\ge 0$ with $\mu >3$. Using Morse theory, we obtain nontrivial solutions of the above equations. Our result complements recent results in [17], where g has to be 3-superlinear at infinity.     

On the global Cauchy problem for the Hartree equation with rapidly decaying initial data

This paper is concerned with the Cauchy problem for the Hartree equation on ${\mathbb{R}}^n,n\in \mathbb{N}$ with the nonlinearity of type $(|?{|}^{?\gamma }?|u{|}^2)u,0<\gamma <n$. It is shown that a global solution with some twisted persistence property exists for data in the space $L^p\cap L^2,1\le p\le 2$ under some suitable conditions on γ and spatial dimension $n\in \mathbb{N}$. It is also shown that the global solution u has a smoothing effect in terms of spatial integrability in the sense that the map $t?u(t)$ is well defined and continuous from $\mathbb{R}?\{0\}$ to $L^{p^{\prime }}$, which is well known for the solution to the corresponding linear Schrödinger equation. Local and global well-posedness results for hat $L^p$-spaces are also presented. The local and global results are proved by combining arguments by Carles–Mouzaoui with a new functional framework introduced by Zhou. Furthermore, it is also shown that the global results can be improved via generalized dispersive estimates in the case of one space dimension.     

Non-Wieferich primes under the abc conjecture

Assuming the abc conjecture, Silverman proved that, for any given positive integer $a?2$, there are $?\log ?x$ primes $p?x$ such that $a^{p?1}?1(\mathrm{mod}{p}^2)$. In this paper, we show that, for any given integers $a?2$ and $k?2$, there still are $?\log ?x$ primes $p?x$ satisfying $a^{p?1}?1(\mathrm{mod}{p}^2)$ and $p\equiv 1(\mathrm{mod}k)$, under the assumption of the abc conjecture. This improves a recent result of Chen and Ding.