We obtain a measure representation for a functional arising in the context of optimal design problems under linear growth conditions. The functional in question corresponds to the relaxation with respect to a pair (\chi,u)$(\chi,u)$, where \chi$\chi$ is the characteristic function of a set of finite perimeter and u$u$ is a function of bounded deformation, of an energy with a bulk term depending on the symmetrized gradient as well as a perimeter term.

In this paper, we prove several results on the exponential decay in L^{2}$L^{2}$ norm of the KdV equation on the real line with localized dampings. First, for the linear KdV equation, the exponential decay holds if and only if the averages of the damping coefficient on all intervals of a fixed length have a positive lower bound. Moreover, under the same damping condition, the exponential decay holds for the (nonlinear) KdV equation with small initial data. Finally, with the aid of certain properties of propagation of regularity in Bourgain spaces for solutions of the associated linear system and the unique continuation property, the exponential decay for the KdV equation with large data holds if the damping coefficient has a positive lower bound on E$E$, where E$E$ is equidistributed over the real line and the complement E^{c}$E^{c}$ has a finite Lebesgue measure.

In this work, we study a high order derivative in time problem. First, we show that there exists a sequence of elements of the spectrum which tends to infinity and therefore, it is ill posed. Then, we prove the uniqueness of solutions for this problem by adapting the logarithmic arguments to this situation. Finally, the results are applied to the backward in time problem for the generalized linear Burgers’ fluid, a couple of heat conduction problems and a viscoelastic model.

In this paper we analyse the global dynamical behaviour of some classical models in the plane. Informally speaking we prove that the folkloric criteria based on the relative positions of the nullclines for Lotka–Volterra systems are also valid in a wide class of discrete systems. The method of proof consists of dividing the plane into suitable positively invariant regions and applying the theory of translation arcs in a subtle manner. Our approach allows us to extend several results of the theory of monotone systems to nonmonotone systems. Applications in models with weak Allee effect, population models for pioneer-climax species, and predator–prey systems are given.

We discuss the dyadic John–Nirenberg space that is a generalization of functions of bounded mean oscillation. A John–Nirenberg inequality, which gives a weak type estimate for the oscillation of a function, is discussed in the setting of medians instead of integral averages. We show that the dyadic maximal operator is bounded on the dyadic John–Nirenberg space and provide a method to construct nontrivial functions in the dyadic John–Nirenberg space. Moreover, we prove that the John–Nirenberg space is complete. Several open problems are also discussed.

For N\geq 2$N\geq 2$, a bounded smooth domain \Omega$\Omega$ in \mathbb {R}^{N}$\mathbb {R}^{N}$, and g_0,\, V_0 \in L^{1}_{loc}(\Omega )$g_0,\, V_0 \in L^{1}_{loc}(\Omega )$, we study the optimization of the first eigenvalue for the following weighted eigenvalue problem:

-\Delta_p \phi + V |\phi|^{p-2}\phi = \lambda g |\phi|^{p-2}\phi \text{ in } \Omega, \quad \phi=0 \text{ on } \partial \Omega, $$-\Delta_p \phi + V |\phi|^{p-2}\phi = \lambda g |\phi|^{p-2}\phi \text{ in } \Omega, \quad \phi=0 \text{ on } \partial \Omega,$$

g$g$

V$V$

g_0$g_0$

V_0$V_0$

(\underline {g},\,\underline {V})$(\underline {g},\,\underline {V})$

(\overline {g},\,\overline {V})$(\overline {g},\,\overline {V})$

g_0$g_0$

V_0$V_0$

p=2$p=2$

Taking the consideration of two-dimensional stochastic Navier–Stokes equations with multiplicative Lévy noises, where the noises intensities are related to the viscosity, a large deviation principle is established by using the weak convergence method skillfully, when the viscosity converges to 0. Due to the appearance of the jumps, it is difficult to close the energy estimates and obtain the desired convergence. Hence, one cannot simply use the weak convergence approach. To overcome the difficulty, one introduces special norms for new arguments and more careful analysis.

Let G$G$ be a compact connected simple Lie group of type (n_{1},\,\ldots,\,n_{l})$(n_{1},\,\ldots,\,n_{l})$, where n_{1}<\cdots < n_{l}$n_{1}<\cdots < n_{l}$. Let \mathcal {G}_k$\mathcal {G}_k$ be the gauge group of the principal G$G$-bundle over S^{4}$S^{4}$ corresponding to k\in \pi _3(G)\cong \mathbb {Z}$k\in \pi _3(G)\cong \mathbb {Z}$. We calculate the mod-p$p$ homology of the classifying space B\mathcal {G}_k$B\mathcal {G}_k$ provided that n_{l}< p-1$n_{l}< p-1$.

In this paper, we consider non-self-adjoint Dirac operators on a finite interval with complex-valued potentials and quasi-periodic boundary conditions. Necessary and sufficient conditions for a set of complex numbers to be the spectrum of the indicated problem are established.

We consider the following inhomogeneous problems

\begin{cases} \epsilon^{2}\mbox{div}(a(x)\nabla u(x))+f(x,u)=0 & \text{ in }\Omega,\\ \frac{\partial u}{\partial \nu}=0 & \text{ on }\partial \Omega,\\ \end{cases} $$\begin{cases} \epsilon^{2}\mbox{div}(a(x)\nabla u(x))+f(x,u)=0 & \text{ in }\Omega,\\ \frac{\partial u}{\partial \nu}=0 & \text{ on }\partial \Omega,\\ \end{cases}$$

\Omega$\Omega$

\mathbb {R}^{N}$\mathbb {R}^{N}$

\epsilon >0$\epsilon >0$

a$a$

L^{1}$L^{1}$

For (X,\,L)$(X,\,L)$ a polarized toric variety and G\subset \mathrm {Aut}(X,\,L)$G\subset \mathrm {Aut}(X,\,L)$ a torus, denote by Y$Y$ the GIT quotient X/\!\!/G$X/\!\!/G$. We define a family of fully faithful functors from the category of torus equivariant reflexive sheaves on Y$Y$ to the category of torus equivariant reflexive sheaves on X$X$. We show, under a genericity assumption on G$G$, that slope stability is preserved by these functors if and only if the pair ((X,\,L),\,G)$((X,\,L),\,G)$ satisfies a combinatorial criterion. As an application, when (X,\,L)$(X,\,L)$ is a polarized toric orbifold of dimension n$n$, we relate stable equivariant reflexive sheaves on certain (n-1)$(n-1)$-dimensional weighted projective spaces to stable equivariant reflexive sheaves on (X,\,L)$(X,\,L)$.

In this study, we consider the viscous compressible Navier–Stokes–Poisson equations, which consist of the balance laws for electron density and moment, and a Poisson equation for the electrostatic potential. The limit of vanishing electron mass of this system with both well/ill-prepared initial data on the whole space is rigorously justified within the framework of local smooth solution. We first make use of the symmetric hyperbolic–parabolic structure of the compressible Navier–Stokes–Poisson equation to obtain uniform estimate in the short time, by which we show uniform existence of local classical solution to the compressible Navier–Stokes–Poisson equation in \mathbb {R}^d(d\geq 1)$\mathbb {R}^d(d\geq 1)$. Further, with uniform estimate of time derivatives, we show the zero-electron-mass limit of the solutions for the compressible Navier–Stokes–Poisson equation with well-prepared initial data in \mathbb {R}^d(d\geq 1)$\mathbb {R}^d(d\geq 1)$ by using Aubin's lemma. A detailed spectral analysis on the linearized system is done so that we are able to prove the zero-electron-mass limit of the solutions with ill-prepared initial data in \mathbb {R}^d(d\geq 3)$\mathbb {R}^d(d\geq 3)$, where the convergence occurs away from the time t=0$t=0$. Finally, note that the dissipation mechanism for the linearized compressible Navier–Stokes–Poisson system is different from that of the compressible Euler equations in Grenier (Commun. Partial Diff. Eqns. 21 (1996), 363–394); Grenier (Commun. Pure Appl. Math. 50 (1997), 821–865); Ukai (J. Math. Kyoto Univ. 26 (1986), 323–331), or that of the compressible Euler–Poisson equations in Ali and Chen (Nonlinearity 24 (2011), 2745–2761), since its eigenvalues are somehow similar to that of heat equation, and the fundamental solution contains a part behaving like the heat kernel, thus a big difficulty is the singularity of the heat kernel at t=0$t=0$.

We prove that, given 2< p<\infty$2< p<\infty$, the Fourier coefficients of functions in L_2(\mathbb {T}, |t|^{1-2/p}\,{\rm d}t)$L_2(\mathbb {T}, |t|^{1-2/p}\,{\rm d}t)$ belong to \ell _p$\ell _p$, and that, given 1< p<2$1< p<2$, the Fourier series of sequences in \ell _p$\ell _p$ belong to L_2(\mathbb {T}, \vert {t}\vert ^{2/p-1}\,{\rm d}t)$L_2(\mathbb {T}, \vert {t}\vert ^{2/p-1}\,{\rm d}t)$. Then, we apply these results to the study of conditional Schauder bases and conditional almost greedy bases in Banach spaces. Specifically, we prove that, for every 1< p<\infty$1< p<\infty$ and every 0\le \alpha <1$0\le \alpha <1$, there is a Schauder basis of \ell _p$\ell _p$ whose conditionality constants grow as (m^{\alpha })_{m=1}^{\infty }$(m^{\alpha })_{m=1}^{\infty }$, and there is an almost greedy basis of \ell _p$\ell _p$ whose conditionality constants grow as ((\log m)^{\alpha })_{m=2}^{\infty }$((\log m)^{\alpha })_{m=2}^{\infty }$.

The paper proves transportation inequalities for probability measures on spheres for the Wasserstein metrics with respect to cost functions that are powers of the geodesic distance. Let \mu$\mu$ be a probability measure on the sphere {\bf S}^n${\bf S}^n$ of the form d\mu =e^{-U(x)}{\rm d}x$d\mu =e^{-U(x)}{\rm d}x$ where {\rm d}x${\rm d}x$ is the rotation invariant probability measure, and (n-1)I+{\hbox {Hess}}\,U\geq {\kappa _U}I$(n-1)I+{\hbox {Hess}}\,U\geq {\kappa _U}I$, where \kappa _U>0$\kappa _U>0$. Then any probability measure \nu$\nu$ of finite relative entropy with respect to \mu$\mu$ satisfies {\hbox {Ent}}(\nu \mid \mu ) \geq (\kappa _U/2)W_2(\nu,\, \mu )^2${\hbox {Ent}}(\nu \mid \mu ) \geq (\kappa _U/2)W_2(\nu,\, \mu )^2$. The proof uses an explicit formula for the relative entropy which is also valid on connected and compact C^\infty$C^\infty$ smooth Riemannian manifolds without boundary. A variation of this entropy formula gives the Lichnérowicz integral.

In this paper, we study divergence properties of the Fourier series on Cantor-type fractal measure, also called the mock Fourier series. We give a sufficient condition under which the mock Fourier series for doubling spectral measure is divergent on a set of strictly positive measure. In particular, there exists an example of the quarter Cantor measure whose mock Fourier sums are not almost everywhere convergent.

In this paper the minimum fundamental gap of a kind of sub-elliptic operator is concerned, we deal with the existence and uniqueness of weak solution for that. We verify that the minimization fundamental gap problem can be achieved by some function, and characterize the optimal function by adopting the differential of eigenvalues.

In this paper, we present explicit and computable error bounds for the asymptotic expansions of the Hermite polynomials with Plancherel–Rotach scale. Three cases, depending on whether the scaled variable lies in the outer or oscillatory interval, or it is the turning point, are considered separately. We introduce the ‘branch cut’ technique to express the error terms as integrals on the contour taken as the one-sided limit of curves approaching the branch cut. This new technique enables us to derive simple error bounds in terms of elementary functions. We also provide recursive procedures for the computation of the coefficients appearing in the asymptotic expansions.

In this work we derive by \Gamma$\Gamma$-convergence techniques a model for brittle fracture linearly elastic plates. Precisely, we start from a brittle linearly elastic thin film with positive thickness \rho$\rho$ and study the limit as \rho$\rho$ tends to 0$0$. The analysis is performed with no a priori restrictions on the admissible displacements and on the geometry of the fracture set. The limit model is characterized by a Kirchhoff-Love type of structure.

In this paper we consider the unfolding of saddle-node

X= \frac{1}{xU_a(x,y)}\Big(x(x^{\mu}-\varepsilon)\partial_x-V_a(x)y\partial_y\Big), $$X= \frac{1}{xU_a(x,y)}\Big(x(x^{\mu}-\varepsilon)\partial_x-V_a(x)y\partial_y\Big),$$

(\varepsilon,\,a)$(\varepsilon,\,a)$

\varepsilon \approx 0$\varepsilon \approx 0$

a$a$

A$A$

{\mathbb {R}}^{\alpha },${\mathbb {R}}^{\alpha },$

\mathcal {T}(s;\varepsilon,\,a)$\mathcal {T}(s;\varepsilon,\,a)$

\partial _s\mathcal {T}(s;\varepsilon,\,a)$\partial _s\mathcal {T}(s;\varepsilon,\,a)$

-\infty$-\infty$

(s,\,\varepsilon )\to (0^{+},\,0)$(s,\,\varepsilon )\to (0^{+},\,0)$

A.$A.$

We consider a class of generalized nonlocal p$p$-Laplacian equations. We find some proper structural conditions to establish a version of nonlocal Harnack inequalities of weak solutions to such nonlocal problems by using the expansion of positivity and energy estimates.