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Jiankang Xia

Publications and source records attributed to Jiankang Xia.

7 recordsLinked to original sources

Some Reverse Hardy-Littlewood-Sobolev Type Inequalities

We establish some sharp reverse Hardy-Littlewood-Sobolev (HLS) type inequalities on \(\mathbb{R}^n\) and \(\mathbb{R}_+^n\). Using an operator representation, we overcome the difficulty that the symmetric double-integral structure is unavailable in the half-space setting. On \(\mathbb{R}^n\), for \(1 \le n < α\), \(\frac{n}α < t < 1\), and \(0 < q < 1\), there holds for nonnegative \(f \) that \[ \|E_αf \|_{L^{t^\prime}(\mathbb{R}^n)} \ge \mathscr{C}(n,α,q,t) \|f \|_{L^1(\mathbb{R}^n)}^γ \|f \|_{L^q(\mathbb{R}^n)}^{1-γ}, \quad γ:= \frac{n - qα- \frac{n}{t^\prime}q}{n(1-q)} \] for some $\mathscr{C}(n,α,q,t)>0$ iff \(q>\frac{n}α\), where \(E_α\) is the extension operator with Riesz kernel and \(t^\prime\) is the conjugate of \(t\). The sharp constant is achieved when \(\frac{n t^\prime}{n + αt^\prime} \le q < 1\). On \(\mathbb{R}_+^n\), with \(2 \le n < α\), \(\frac{n}α < t < 1\), and \(0 < q < 1\), we show for nonnegative \(f \) that \[ \|\widetilde{E}_αf \|_{L^{t^\prime}(\mathbb{R}_+^n)} \ge\widetilde{\mathscr{C}}(n,α,q,t) \|f\|_{L^1(\partial \mathbb{R}_+^n)}^{\widetildeγ} \|f\|_{L^q(\partial \mathbb{R}_+^n)}^{1-\widetildeγ}, \quad \widetildeγ := \frac{(n-1) - q(α-1) - \frac{n}{t^\prime}q}{(n-1)(1-q)}, \] for some $\widetilde{\mathscr{C}}(n,α,q,t)>0$ iff \(q > \frac{n-1}{α-1}\), where \(\widetilde{E}_α\) is the extension operator with Poisson-type kernel. The sharp constant is achieved when \(\frac{t^\prime(n-1)}{n + t^\prime(α-1)} \le q < 1\). We further extend results to \(q\ge1\). The proofs use rearrangement inequalities, the sharp Carlson--Levin inequality, and refined pointwise lower bounds for the Riesz and Poisson-type potentials. Our results unify and extend the classical reverse HLS inequalities, especially on \(\mathbb{R}_+^n\).

math.FA

Normalized groundstates for mixed $(p,2)$-Laplacian equations in $\mathbb R^2$ with exponential critical growth

We investigate normalized groundstates for mixed $(p,2)$-Laplacian equations \begin{align*} \begin{cases} -Δ_p u-Δu+λu=f(u) & \text{in } \mathbb{R}^2, \displaystyle \int_{\mathbb{R}^2}|u|^2\,\mathrm{d}x=m, u\in H^1(\mathbb{R}^2)\cap D^{1,p}(\mathbb{R}^2), \end{cases} \end{align*} where $Δ_p$ denotes the $p$-Laplacian with $1 0$. Notably, our approach works independently of the sign of the Lagrange multiplier $λ$, thereby surmounting the fundamental barrier in recovering compactness for mixed Laplacian problems.

math.AP

Saddle solutions for the Choquard equation with a general nonlinearity

In the spirit of Berestycki and Lions, we prove the existence of saddle type nodal solutions for the Choquard equation \[ -Δu + u= \big(I_α\ast F(u)\big)F'(u)\qquad \text{ in }\;\mathbb{R}^N \] where $N\geq 2$ and $I_α$ is the Riesz potential of order $α\in (0,N)$. Without any compact setting, we construct saddle solutions in a unified way for the Choquard equation whose nodal domains are of cone shapes demonstrating Coxeter's symmetric configurations in $\mathbb R^N$. Moreover, if $F'$ is odd and has constant sign on $(0,+\infty)$, then the saddle solution maintains signed on the fundamental domain of the corresponding Coxeter group and receives opposite signs on any two adjacent domains. These results further complete the variational framework in constructing sign-changing solutions for the Choquard equation but still require a quadratic or super-quadratic growth on $F$ near the origin.

math.AP

Saddle solutions for the fractional Choquard equation

We study the saddle solutions for the fractional Choquard equation \begin{align*} (-Δ)^{s}u+ u=(K_α\ast|u|^{p})|u|^{p-2}u, \quad x\in \mathbb{R}^N \end{align*} where $s\in(0,1)$, $N\geq 3$ and $K_α$ is the Riesz potential with order $α\in (0,N)$. For every Coxeter group $G$ with rank $1\leq k\leq N$ and $p\in[2,\frac{N+α}{N-2s})$, we construct a $G$-saddle solution with prescribed symmetric nodal configurations. This is a counterpart for the fractional Choquard equation of saddle solutions to the Choquard equation and further completes the existence of non-radial sign-changing solutions for this doubly nonlocal equation.

math.AP

Groundstates for a local nonlinear perturbation of the Choquard equations with lower critical exponent

We prove the existence of ground state solutions by variational methods to the nonlinear Choquard equations with a nonlinear perturbation \[ -Δu+ u=\big(I_α*|u|^{\fracα{N}+1}\big)|u|^{\fracα{N}-1}u+f(x,u)\qquad \text{ in } \mathbb{R}^N \] where $N\geq 1$, $I_α$ is the Riesz potential of order $α\in (0, N)$, the exponent $\fracα{N}+1$ is critical with respect to the Hardy--Littlewood--Sobolev inequality and the nonlinear perturbation $f$ satisfies suitable growth and structural assumptions.

math.AP

Standing waves with a critical frequency for nonlinear Choquard equations

In this paper, we study the nonlocal Choquard equation $$ -\varepsilon^2 Δu_\varepsilon + V u_\varepsilon= (I_α* |u_\varepsilon|^p)|u_\varepsilon|^{p-2}u_\varepsilon $$ where $N\geq 1$, $I_α$ is the Riesz potential of order $α\in (0, N)$ and $\varepsilon>0$ is a parameter. When the nonnegative potential $V\in C (\mathbb{R}^N)$ achieves $0$ with a homogeneous behaviour or on the closure of an open set but remains bounded away from $0$ at infinity, we show the existence of groundstate solutions for small $\varepsilon>0$ and exhibit the concentration behaviour as $\varepsilon\to 0$.

math.AP

Choquard equations under confining external potentials

We consider the nonlinear Choquard equation $$ -Δu+V u=(I_α\ast \vert u\vert ^p)\vert u\vert ^{p-2}u \qquad \text{ in } \mathbb{R}^N $$ where $N\geq 1$, $I_α$ is the Riesz potential integral operator of order $α\in (0, N)$ and $p > 1$. If the potential $ V \in C (\mathbb{R}^N; [0,+\infty)) $ satisfies the confining condition $$ \liminf\limits_{\vert x\vert \to +\infty}\frac{V(x)}{1+\vert x\vert ^{\frac{N+α}{p}-N}}=+\infty, $$ and $\frac{1}{p} > \frac{N - 2}{N + α}$, we show the existence of a groundstate, of an infinite sequence of solutions of unbounded energy and, when $p \ge 2$ the existence of least energy nodal solution. The constructions are based on suitable weighted compact embedding theorems. The growth assumption is sharp in view of a Pohožaev identity that we establish.

math.AP