Analysis of PDEs
☆ On Courant-type bounds and spectral partitioning via Neumann domains on quantum graphs
We study the structure of eigenfunctions of the Laplacian on quantum graphs,
with a particular focus on Morse eigenfunctions via nodal and Neumann domains.
Building on Courant-type arguments, we establish upper bounds for the number of
nodal points and explore conditions under which Neumann domains of
eigenfunctions correspond to minimizers to a class of spectral partition
problems often known as spectral minimal partitions. The main focus will be the
analysis on tree graphs, where we characterize the spectral energies of such
partitions and relate them to the eigenvalues of the Laplacian under genericity
assumptions. Notably, we introduce a notion analogous to Courant-sharpness for
Neumann counts and demonstrate when spectral minimal partitions coincide with
partitions formed by Neumann domains of eigenfunctions.
☆ Vorticity blow-up for the 3D incompressible Euler equations
In this paper, we study the finite-time blow-up for classical solutions of
the 3D incompressible Euler equations with low-regularity initial vorticity.
Applying the self-similar method and stability analysis of the self-similar
system in critical Sobolev space, we prove that the vorticity of the
axi-symmetric 3D Euler equations develops a finite-time singularity with
certain scaling indices. Furthermore, we investigate the time integrability of
the solutions. The proof is based on the new observations for the null
structure of the transport term, and the parameter stability of the fundamental
self-similar models.
☆ Global existence and decay of small solutions in a viscous half Klein-Gordon equation
We establish global existence and decay of solutions of a viscous half
Klein-Gordon equation with a quadratic nonlinearity considering initial data,
whose Fourier transform is small in L1 cap Linfty. Our analysis relies on the
observation that nonresonant dispersive effects yield a transformation of the
quadratic nonlinearity into a subcritical nonlocal quartic one, which can be
controlled by the linear diffusive dynamics through a standard L1 - Linfty
argument. This transformation can be realized by applying the normal form
method of Shatah or, equivalently, through integration by parts in time in the
associated Duhamel formula.
comment: 17 pages
☆ Perturbation theory of the compressible Navier-Stokes equations and its application
In this article, a perturbation theory of the compressible Navier-Stokes
equations in $\mathbb{R}^n$ $(n \geq 3)$ is studied to investigate decay
estimate of solutions around a non-constant state. As a concrete problem,
stability is considered for a perturbation system from a stationary solution
$u_\omega$ belonging to the weak $L^n$ space. Decay rates of the perturbation
including $L^\infty$ norm are obtained which coincide with those of the heat
kernel. The proof is based on deriving suitable resolvent estimates with
perturbation terms in the low frequency part having a parabolic spectral curve.
Our method can be applicable to dispersive hyperbolic systems like wave
equations with strong damping. Indeed, a parabolic type decay rate of a
solution is obtained for a damped wave equation including variable coefficients
which satisfy spatial decay conditions.
☆ Low-complexity approximations with least-squares formulation of the time-dependent Schr{ö}dinger equation
We propose new methods designed to numerically approximate the solution to
the time dependent Schr{\"o}dinger equation, based on two types of ansatz:
tensors, and approximation by a linear combination of gaussian wave packets. In
both cases, the method can be seen as a restricted optimization problem, which
can be solved by adapting either the Alternating Least Square algorithm in the
tensor case, or some greedy algorithm in the gaussian wavepacket case. We also
discuss the efficiency of both approaches.
☆ Mathematical Study of Reaction-Diffusion in Congested Crowd Motion
This paper establishes existence, uniqueness, and an L^1-comparison principle
for weak solutions of a PDE system modeling phase transition reaction-diffusion
in congested crowd motion. We consider a general reaction term and mixed
homogeneous (Dirichlet and Neumann) boundary conditions. This model is
applicable to various problems, including multi-species diffusion-segregation
and pedestrian dynamics with congestion. Furthermore, our analysis of the
reaction term yields sufficient conditions combining the drift with the
reaction that guarantee the absence of congestion, reducing the dynamics to a
constrained linear reaction-transport equation.
☆ Degenerate Elliptic PDEs on a Network with Kirchhoff Conditions
In this article, we are interested in semilinear, possibly degenerate
elliptic equations posed on a general network, with nonlinear Kirchhoff-type
conditions for its interior vertices and Dirichlet boundary conditions for the
boundary ones. The novelty here is the generality of the equations posed on
each edge that is incident to a particular vertex, ranging from first-order
equations to uniformly elliptic ones. Our main result is a strong comparison
principle, i.e., a comparison result between discontinuous viscosity sub and
supersolutions of such problems, from which we conclude the existence and
uniqueness of a continuous viscosity by Perron's method. Further extensions are
also discussed.
☆ Wave maps from circle to Riemannian manifold: global controllability is equivalent to homotopy
We study wave maps from the circle to a general compact Riemannian manifold.
We prove that the global controllability of this geometric equation is
characterized precisely by the homotopy class of the data. As a remarkable
intermediate result, we establish uniform-time global controllability between
steady states, providing a partial answer to an open problem raised by Dehman,
Lebeau and Zuazua (2003). Finally, we obtain quantitative exponential stability
around closed geodesics with negative sectional curvature. This work highlights
the rich interplay between partial differential equations, differential
geometry, and control theory.
☆ Normalized solutions of quasilinear Schrödinger equation with Sobolev critical exponent on star-shaped bounded domains
In this paper, we consider a quasilinear Schr\"odinger equation with critical
exponent on bounded domains. Via a dual approach, we establish the existence of
two positive normalized solutions: one is a ground state and the other is a
mountain pass solution.
☆ Inverse scattering for the fractional Schrödinger equation
This article is devoted to studying the inverse scattering for the fractional
Schr\"{o}dinger equation, and in particular we solve the Born approximation
problem. Based on the ($p$,$q$)-type resolvent estimate for the fractional
Laplacian, we derive an expression for the scattering amplitude of the
scattered solution of the fractional Schr\"{o}dinger equation. We prove the
uniqueness of the potential using the scattering amplitude data.
comment: 19 pages
☆ Ill-posedness in $B^s_{p,\infty}$ of the Euler equations: Non-continuous dependence
In this paper, we solve an open problem left in the monographs
\cite[Bahouri-Chemin-Danchin, (2011)]{BCD}. Precisely speaking, it was obtained
in \cite[Theorem 7.1 on pp293, (2011)]{BCD} the existence and uniqueness of
$B^s_{p,\infty}$ solution for the Euler equations. We furthermore prove that
the solution map of the Euler equation is not continuous in the Besov spaces
from $B^s_{p,\infty}$ to $L_T^\infty B^s_{p,\infty}$ for $s>1+d/p$ with $1\leq
p\leq \infty$ and in the H\"{o}lder spaces from $C^{k,\alpha}$ to $L_T^\infty
C^{k,\alpha}$ with $k\in \mathbb{N}^+$ and $\alpha\in(0,1)$, which later covers
particularly the ill-posedness of $C^{1,\alpha}$ solution in \cite[Trans. Amer.
Math. Soc., (2018)]{MYtams}. Beyond purely technical aspects on the choice of
initial data, a remarkable novelty of the proof is the construction of an
approximate solution to the Burgers equation.
☆ Global Existence and Incompressible Limit for the Three-Dimensional Axisymmetric Compressible Navier-Stokes Equations with Large Bulk Viscosity and Large Initial Data
In this paper, we study the three-dimensional axisymmetric compressible
Navier-Stokes equations with slip boundary conditions in a cylindrical domain
excluding the axis. We establish the global existence and exponential decay of
weak, strong, and classical solutions with large initial data and vacuum, under
the assumption that the bulk viscosity coefficient is sufficiently large.
Moreover, we demonstrate that as the bulk viscosity coefficient tends to
infinity, the solutions of the compressible Navier-Stokes equations converge to
those of the inhomogeneous incompressible Navier-Stokes equations.
comment: arXiv admin note: substantial text overlap with arXiv:2509.11260
♻ ☆ Delayed parabolic regularity for curve shortening flow
Given two curves bounding a region of area $A$ that evolve under curve
shortening flow, we propose the principle that the regularity of one should be
controllable in terms of the regularity of the other, starting from time
$A/\pi$. We prove several results of this form and demonstrate that no estimate
can hold before that time. As an example application, we construct solutions to
graphical curve shortening flow starting with initial data that is merely an
$L^1$ function.
comment: v1 was not submitted. v2 has numerous adjustments and improvements to
the exposition
♻ ☆ A double-phase Neumann problem with $p=1$
We study a double-phase Neumann problem with non-homogeneous boundary
conditions, where the lowest exponent $p$ is equal to 1. The existence of a
solution is established as the limit of solutions to corresponding double-phase
problems with $p>1$. We also provide a variational characterization of the
limit.
comment: 18 pages
♻ ☆ Uniqueness in determining multidimensional domains with unknown initial data
This paper addresses several geometric inverse problems for some linear
parabolic systems where the initial data (and sometimes also the coefficients
of the equations) are unknown.
The goal is to identify a subdomain within a multidimensional set.
The non-homogeneous part of the equation is expressed as a function
satisfying some specific assumptions near a positive time.
We establish uniqueness results by incorporating observations that can be on
a part of the boundary or in an interior (small) domain.
Through this process, we also derive information about the initial data.
The main tools required for the proofs include semigroup theory, unique
continuation and time analyticity results
♻ ☆ Upper bound on heat kernels of finite particle systems of Keller-Segel type
We obtain an upper bound on the heat kernel of the Keller-Segel finite
particle system that exhibits blow up effects. The proof exploits a connection
between Keller-Segel finite particles and certain non-local operators. The
latter allows to address some aspects of the critical behaviour of the
Keller-Segel system resulting from its two-dimensionality.
comment: References added, a few typos fixed
♻ ☆ On the singular set of $\operatorname{BV}$ minimizers for non-autonomous functionals
We investigate regularity properties of minimizers for non-autonomous convex
variational integrands $F(x, \mathrm{D} u)$ with linear growth, defined on
bounded Lipschitz domains $\Omega \subset \mathbb{R}^n$. Assuming appropriate
ellipticity conditions and H\"older continuity of $\mathrm{D}_zF(x,z)$ with
respect to the first variable, we establish higher integrability of the
gradient of minimizers and provide bounds on the Hausdorff dimension of the
singular set of minimizers.
comment: Version 2, 26 pages, 1 figure. Final version to appear in
Communications in Contemporary Mathematics
♻ ☆ The Ground State of a Cubic-quintic Nonlinear Schrödinger Equation with Radial Potential in the Thomas-Fermi Limit
We focus on the ground state of the cubic-quintic nonlinear Schr\"{o}dinger
energy functional \begin{gather*}
\begin{aligned}
{E}(\varphi)=\frac{1}{2}\int_{\mathbb{R}^d}\left(|\nabla
\varphi|^2+V(x)|\varphi|^2\right)\,dx
\pm\frac{1}{4}\int_{\mathbb{R}^d}|\varphi|^4\,dx
+\frac{1}{6}\int_{\mathbb{R}^d}|\varphi|^6\,dx, (d=1,2,3)
\end{aligned} \end{gather*}
under the mass constraint $\int_{\mathbb{R}^d}|\varphi|^2\,dx=N$, where $N$
can be viewed as particle number, and $V(x)$ behaves like $C|x|^p (p\geq 2)$ as
$|x|\rightarrow +\infty$, including the harmonic potential. When $N\rightarrow
+\infty$, we show that up to a suitable scaling the ground state $\varphi_N$
would convergence strongly in some $L^q(\mathbb{R}^d)$ space to a Thomas-Fermi
minimizer, this limit can be referred to as the \emph{Thomas-Fermi limit}. The
limit Thomas-Fermi profile has compact support, given by
$u^{TF}(x)=\left[\mu^{TF}-C_0|x|^p\right]^{\frac{1}{4}}_{+}$, where $\mu^{TF}$
is a suitable Lagrange multiplier with exact value. We find that, similar to
the asymptotic analysis in [J. Funct. Anal. 260 (2011), 2387-2406.] and [Arch.
Ration. Mech. Anal. 217 (2015), 439-523.] for Gross-Pitaevskii energy in the
Thomas-Fermi limit where a small parameter $\varepsilon$ tends to 0, there also
has a steep \emph{corner layer} near the boundary of compact support of
$u^{TF}(x)$, in which the ground state has irregular behavior as $N\rightarrow
+\infty$. Finally, we establish a new energy method to obtain the
$L^\infty$-convergence rates of ground states $\varphi_N$ inside the corner
layer and outside corner layer respectively, this method may be applicable to
other general nonlinearities.
comment: 39 pages
♻ ☆ Construction of solutions for a critical elliptic system of Hamiltonian type
We consider the following nonlinear elliptic system of Hamiltonian type with
critical exponents: \begin{equation*}\left\{\begin{aligned} &-\Delta u +
V(|y'|,y'') u = v^p, \;\; \text{in} \;\; \mathbb{R}^N,\\ &-\Delta v +
V(|y'|,y'') v = u^q, \;\; \text{in} \;\; \mathbb{R}^N,\\ &u, v > 0 , (u,v) \in
(\dot{W}^{2,\frac{p+1}{p}} (\mathbb{R}^N) \cap L^2(\mathbb{R}^N)) \times
(\dot{W}^{2,\frac{q+1}{q}} (\mathbb{R}^N) \cap L^2(\mathbb{R}^N))
,\end{aligned}\right. \end{equation*} where $(y', y'') \in \mathbb{R}^2 \times
\mathbb{R}^{N-2}$ and $V(|y'|, y'')\not\equiv 0$ is a bounded non-negative
function in $\mathbb{R}_+\times \mathbb{R}^{N-2}$, $p,q>1$ satisfying
$$\frac{1}{p+1}+\frac{1}{q+1}=\frac{N-2}{N}.$$ By using a finite reduction
argument and local Pohozaev identities, under the assumption that $N\geq 5$,
$(p,q)$ lies in the certain range and $r^2V(r,y'')$ has a stable critical
point, we prove that the above problem has infinitely many solutions whose
energy can be made arbitrarily large.
♻ ☆ Optimal Runge approximation for nonlocal wave equations and unique determination of polyhomogeneous nonlinearities
The main purpose of this article is to establish the Runge-type approximation
in $L^2(0,T;\widetilde{H}^s(\Omega))$ for solutions of linear nonlocal wave
equations. To achieve this, we extend the theory of very weak solutions for
classical wave equations to our nonlocal framework. This strengthened Runge
approximation property allows us to extend the existing uniqueness results for
Calder\'on problems of linear and nonlinear nonlocal wave equations in our
earlier works. Furthermore, we prove unique determination results for the
Calder\'on problem of nonlocal wave equations with polyhomogeneous
nonlinearities.
comment: 38 pages