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Giao Ky Duong

Publications and source records attributed to Giao Ky Duong.

8 recordsLinked to original sources

Finite-Rank Optimizers for the mass--supercritical Lieb--Thirring and Hardy--Lieb--Thirring Inequalities

We establish the existence of finite-rank operators for an interpolation version of the Lieb--Thirring inequality in the mass--supercritical case, thereby extending a result of Hong, Kwon, and Yoon in 2019 to the full parameter regime. Our method also applies to the Hardy--Lieb--Thirring inequality, where the existence of optimizers faces additional difficulties due to the singularity of the inverse-square potential.

math-ph↗

Flat blow-up solutions for the complex Ginzburg Landau equation

In this paper, we consider the complex Ginzburg-Landau equation $$ \partial_t u = (1 + i β) Δu + (1 + i δ) |u|^{p-1}u - αu, \quad \text{where } β, δ, α\in \mathbb{R}. $$ The study focuses on investigating the finite-time blow-up phenomenon, which remains an open question for a broad range of parameters, particularly for \(β\) and \(δ\). Specifically, for a fixed \(β\in \mathbb{R}\), the existence of finite-time blow-up solutions for arbitrarily large values of \( |δ| \) is still unknown. According to a conjecture made by Popp et al. \cite{POPphd98}, when \(β= 0\) and \(δ\) is large, blow-up does not occur for \textit{generic initial data}. In this paper, we show that their conjecture is not valid for all types of initial data, by presenting the existence of blow-up solutions for \(β= 0\) and any \(δ\in \mathbb{R}\) with different types of blowup.

math.AP↗

Cwikel-Lieb-Rozenblum type inequalities for Hardy-Schrödinger operator

We prove a Cwikel-Lieb-Rozenblum type inequality for the number of negative eigenvalues of the Hardy-Schrödinger operator $-Δ- (d-2)^2/(4|x|^2) -W(x)$ on $L^2(\mathbb{R}^d)$. The bound is given in terms of a weighted $L^{d/2}-$norm of $W$ which is sharp in both large and small coupling regimes. We also obtain a similar bound for the fractional Laplacian.

math-ph↗

Modulation theory for the flat blowup solutions of nonlinear heat equation

In this paper, we revisit the proof of the existence of a solution to the semilinear heat equation in one space dimension with a at blowup profile, already proved by Bricmont and Kupainen together with Herrero and Velázquez. Though our approach relies on the well celebrated method, based on the reduction of the problem to a finite dimensional one, then the use of a topological shooting method to solve the latter, the novelty of our approach lays in the use of a modulation technique to control the projection of the zero eigenmode arising in the problem. Up to our knowledge, this is the first time where modulation is used with this kind of profiles. We do hope that this simplifies the argument.

math.AP↗

Profile of touch-down solution to a nonlocal MEMS model

In this paper, we are interested in the mathematical model of MEMS devices which is presented by the following equation on $(0,T) \times Ω:$ \begin{eqnarray*} \partial_t u = Δu +\displaystyle \frac{λ}{ (1-u)^2 \left( 1 +\displaystyle γ\int_Ω \frac{1}{1-u} dx \right)^2}, \quad 0 \leq u <1, \end{eqnarray*} where $Ω$ is a bounded domain in $\mathbb{R}^n$ and $λ, γ> 0$. In this work, we have succeeded to construct a solution which quenches in finite time T only at one interior point $a \in Ω$. In particular, we give a description of the quenching behavior according to the following final profile $$ 1 - u(x,T) \sim θ^*\left[ \frac{|x-a|^2}{|\ln|x-a||} \right]^\frac{1}{3} \text{ as } x \to a, θ^* > 0.$$ The construction relies on some connection between the quenching phemonenon and the blowup phenomenon. More precisely, we change our problem to the construction of a blowup solution for a related PDE and describe its behavior. The proof relies on two main steps: A reduction to a finite dimensional problem and a topological argument based on Index theory. The highlight of this work is that we handle the nonlocal integral term in the above equation. The interpretation of the finite dimensional parameters in terms of the blowup point and the blowup time allows to derive the stability of the constructed solution with respect to initial data.

math.AP↗

A blowup solution of a complex semi-linear heat equation with an irrational power

In this paper, we consider the following semi-linear complex heat equation \begin{eqnarray*} \partial_t u = Δu + u^p, u \in \mathbb{C} \end{eqnarray*} in $\mathbb{R}^n,$ with an arbitrary power $p,$ $ p > 1$. In particular, $p$ can be non integer and even irrational. We construct for this equation a complex solution $u = u_1 + i u_2$, which blows up in finite time $T$ and only at one blowup point $a.$ Moreover, we also describe the asymptotics of the solution by the following final profiles: \begin{eqnarray*} u(x,T) &\sim & \left[ \frac{(p-1)^2 |x-a|^2}{ 8 p |\ln|x-a||}\right]^{-\frac{1}{p-1}},\\ u_2(x,T) &\sim & \frac{2 p}{(p-1)^2} \left[ \frac{ (p-1)^2|x-a|^2}{ 8p |\ln|x-a||}\right]^{-\frac{1}{p-1}}\frac{1}{ |\ln|x-a||} > 0 , \text{ as } x \to a. \end{eqnarray*} In addition to that, since we also have $u_1 (0,t) \to + \infty$ and $u_2(0,t) \to - \infty$ as $t \to T,$ the blowup in the imaginary part shows a new phenomenon unkown for the standard heat equation in the real case: a non constant sign near the singularity, with the existence of a vanishing surface for the imaginary part, shrinking to the origin. In our work, we have succeeded to extend for any power $p$ where the non linear term $u^p$ is not continuous if $ p$ is not integer. In particular, the solution which we have constructed has a positive real part. We study our equation as a system of the real part and the imaginary part $u_1$ and $u_2$. Our work relies on two main arguments: the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to get the conclusion.

math.AP↗

Profile for the imaginary part of a blowup solution for a complex-valued seminar heat equation

In this paper, we consider the following complex-valued semilinear heat equation \begin{eqnarray*} \partial_t u = Δu + u^p, u \in \mathbb{C}, \end{eqnarray*} in the whole space $\mathbb{R}^n$, where $ p \in \mathbb{N}, p \geq 2$. We aim at constructing for this equation a complex solution $u = u_1 + i u_2$, which blows up in finite time $T$ and only at one blowup point $a$, with the following estimates for the final profile \begin{eqnarray*} u(x,T) &\sim & \left[ \frac{(p-1)^2 |x-a|^2}{ 8 p |\ln|x-a||}\right]^{-\frac{1}{p-1}}, u_2(x,T) &\sim & \frac{2 p}{(p-1)^2} \left[ \frac{ (p-1)^2|x-a|^2}{ 8p |\ln|x-a||}\right]^{-\frac{1}{p-1}}\frac{1}{ |\ln|x-a||} , \text{ as } x \to a. \end{eqnarray*} Note that the imaginary part is non-zero and that it blows up also at point $a$. Our method relies on two main arguments: the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to get the conclusion. Up to our knowledge, this is the first time where the blowup behavior of the imaginary part is derived in multi-dimension.

math.AP↗