A Characterization for Windowed Fourier Orthonormal Basis with Compact Support

Let g(x) ∈L ²(R) and ğ(ω) be the Fourier transform of g(x). Define g _mn (x) = e ^imx g(x−2πn). In this paper we shall give a sufficient and necessary condition under which {g _mn (x)} constitutes an orthonormal basis of L ²(R) for compactly supported g(ω) or ˘(ω). Received March 25, 1999, Revised November 5, 1999, Accepted September 6, 2000     

Stability of Standing Waves for Nonlinear Schrödinger Equations with Inhomogeneous Nonlinearities

The effect of inhomogeneity of nonlinear medium is discussed concerning the stability of standing waves e^{i ω t}ϕ_ω(x) for a nonlinear Schr?dinger equation with an inhomogeneous nonlinearity V (x)|u|^{p − 1}u, where V (x) is proportional to the electron density. Here, ω > 0 and ϕ_ω(x) is a ground state of the stationary problem. When V (x) behaves like |x|^−b at infinity, where 0 < b < 2, we show that e^{i ω t}ϕ_ω(x) is stable for p < 1 + (4 − 2b)/n and sufficiently small ω > 0. The main point of this paper is to analyze the linearized operator at standing wave solution for the case of V (x) = |x|^−b. Then, this analysis yields a stability result for the case of more general, inhomogeneous V (x) by a certain perturbation method. Communicated by Bernard Helffer submitted 14/07/04, accepted 28/02/05     

Global smooth solutions to a class of semilinear wave equaiions with strong nonlinearities

We consider the Cauchy problem for semilinear wave equationsu _tt−Δu=g(u) in 3+1 dimensions with smooth but possibly large data. Ifg isC ^2,α and bounded from above everywhere and from below for negative arguments the existence of a global classical solution is shown. If moreoverg is nonpositive and vanishes at least of order 2+∈ at the origin and if the data decay sufficiently rapidly at infinity the scattering operator exists.     

Certain asymptotic expansions for laguerre polynomials and Charlier polynomials

Here proposed are certain asympotic expansion formulas for L _n ^(∞-1) (λz) and C _n ^(∞) (λz) in which 0<w=0(λ) and C_n/(^w)(λz), z being a complex number. Also presented are certain estimates for the remainders (error bounds) of the asymptotic expansions within the regions D₁(-∞<R_ez<=1/2(ω/λ) and D₂(1/2(ω/λ)<=Re_z<∞), respectively. Supported by NSERC (Canada) and also by the National Natural Science Foundation of China.     

Instability of Standing Wave for the Klein–Gordon–Hartree Equation

The instability property of the standing wave uω(t, x) = eiωtφ(x) for the Klein–Gordon– Hartree equation     

Embedding of Hpω in the class eL

We obtain the necessary conditions for the embedding H _p ^ω ⊂ e ^L (1≤p∞) with convex modulus of continuity ω in terms of this modulus. In the case p=1 these conditions are also sufficient.     

Quasi-periodic Solutions of Completely Resonant Wave Equations with Quasi-periodically forced Vibrations

In this paper, we provide the existence of quasi-periodic solutions with two frequencies for a class of completely resonant nonlinear wave equations with quasi-periodically forced vibrations under the spatial periodic boundary conditions. We consider the frequencies vector (ω ₁,ω ₂) near the linear system. The proofs are based on the Variational Lyapunov-Schmidt reduction and Linking Theorem.     

A method for indefinite integration of oscillatory and singular functions

We propose a general method for computing indefinite integrals of the form

On the exponent of tensor categories coming from finite groups

We describe the exponent of a group-theoretical fusion category C = C(G, ω, F, α) associated to a finite group G in terms of group cohomology. We show that the exponent of C divides both e(ω)expG and (expG)², where e(ω) is the cohomological order of the 3-cocycle ω. In particular, expC divides (dim C)². This work was partially supported by CONICET, Fundación Antorchas, Agencia Córdoba Ciencia, ANPCyT and Secyt (UNC).     

On a superatomic Boolean algebra which is not generated by a well-founded sublattice

Let b denote the unboundedness number of ω^ω. That is, b is the smallest cardinality of a subset such that for everyg∈ω^ω there isf ∈ F such that {n: g(n) ≤ f(n)}is infinite. A Boolean algebraB is wellgenerated, if it has a well-founded sublatticeL such thatL generatesB. We show that it is consistent with ZFC that , and there is a Boolean algebraB such thatB is not well-generated, andB is superatomic with cardinal sequence 〈ℵ₀, ℵ₁, ℵ₁, 1〉. This result is motivated by the fact that if the cardinal sequence of a Boolean algebraB is 〈ℵ₀, ℵ₀, λ, 1〉, andB is not well-generated, then λ≥b.     

k-NN METHOD IN PARTIAL LINEAR MODEL UNDER RANDOM CENSORSHIP

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Two-Dimensional Graphs Moving by Mean Curvature Flow

A surface Σ is a graph in ?⁴ if there is a unit constant 2-form ω on ?⁴ such that <e ₁∧e ₂, ω≥v ₀>0 where {e ₁, e ₂} is an orthonormal frame on Σ. We prove that, if $ \vartheta _{0} \geqslant \frac{1} {{{\sqrt 2 }}} A surface Σ is a graph in ℝ⁴ if there is a unit constant 2-form ω on ℝ⁴ such that <e ₁∧e ₂, ω>≥v ₀>0 where {e ₁, e ₂} is an orthonormal frame on Σ. We prove that, if v ₀≥ on the initial surface, then the mean curvature flow has a global solution and the scaled surfaces converge to a self-similar solution. A surface Σ is a graph in M ₁×M ₂ where M ₁ and M ₂ are Riemann surfaces, if <e ₁∧e ₂, ω₁>≥v ₀>0 where ω₁ is a K?hler form on M ₁. We prove that, if M is a K?hler-Einstein surface with scalar curvature R, v ₀≥ on the initial surface, then the mean curvature flow has a global solution and it sub-converges to a minimal surface, if, in addition, R≥0 it converges to a totally geodesic surface which is holomorphic. Received July 25, 2001, Accepted October 11, 2001     

A construction of weakly inverse semigroups

Let S° be an inverse semigroup with semilattice biordered set E° of idempotents and E a weakly inverse biordered set with a subsemilattice Ep = { e ∈ E ｜ arbieary f ∈ E, S（f , e） loheain in w（e）} isomorphic to E° by θ：Ep→E°. In this paper, it is proved that if arbieary f, g ∈E, f ←→ g→→ f°θD^s° g°θand there exists a mapping φ from Ep into the symmetric weakly inverse semigroup P J（E∪ S°） satisfying six appropriate conditions, then a weakly inverse semigroup ∑ can be constructed in P J（S°）, called the weakly inverse hull of a weakly inverse system （S°, E, θ, φ） with I（∑） ≌ S°, E（∑） ∽- E. Conversely, every weakly inverse semigroup can be constructed in this way. Furthermore, a sufficient and necessary condition for two weakly inverse hulls to be isomorphic is also given.     

On some congruence with application to exponential sums

We will study the solution of a congruence,x ≡g ^1/2)ωg(2 ⁿ ) mod 2 ⁿ , depending on the integersg andn, where ω _g (2 ⁿ ) denotes the order ofg modulo 2 ⁿ . Moreover, we introduce an application of the above result to the study of an estimation of exponential sums.     

High harmonic generation in a two-color field composed of a pump field and a weak subsidiary high frequency field

“Coherent control of high-harmonic generation in a two-color field” has been widely concerned. Using split-operator algorithm, we have calculated the high-harmonic generation for helium ion He+ in a two-color field which is composed of a driving field and a weak subsidiary high frequency field (Is=I0/100, （ω,13ω), …(ω, 120ω)) and found that such a field can produce much higher harmonic intensity, typically increasing the harmonics corresponding to the incident frequency of the subsidiary field. The different effects coming from the different subsidiary fields are calculated and analyzed. It is indicated that one of the important underlying mechanisms is high frequency photon induced radiation.     

Spectre de l'opérateur de transfert en dimension 1

We study spectral properties of a transfer operator ℳΦ(x)=∑_ω g _ω(x)Φ(ψ_ω x) acting on functions of bounded variation. Using a symmetrical integral, we first obtain bounds on its spectral and essential spectral radii. We then consider the dynamical determinant Det^#(Id +zℳ). Our main theorem generalizes to discontinuous weights the result of Baladi and Ruelle (for continuous weights) on the link between zeroes of the sharp determinant and eigenvalues of the transfer operator. The proof is based on regularizing the weights and uses a (new) spectral result giving the surjectivity of some applications between eigenspaces of operators. Received: 8 May 2001     

An information geometry algorithm for distribution control

In this paper, we consider the problem of distribution control from the viewpoint of information geometry. Different from most existing models used in stochastic control, it is assumed that the control input directly affects the distribution of the system output in probability sense. Here, we set up a new manifold (S), meanwhile the B-spline manifold (B) and the system output manifold (M) can be referred to as its submanifolds. We give an information geometrical algorithm which can be called as geodesic-projection algorithm using the properties of manifold. In the geodesic step, we can obtain the geodesic equation from the initial point V₀ = (ω₁₀, ω₂₀, ··· , ω_(n−1)0) to the specified point V_g = (ω_1g, ω_2g, ··· , ω_(n−1)g) in B. This gives us an optimal trajectory for the points changing along in B. In the projection step, we project the sample points selected from the geodesic onto M. The coordinates of the projections in M give the trajectory of the control input u.     

decay problem for the dissipative wave equation in odd dimensions

Consider the Cauchy problem in odd dimensions for the dissipative wave equation: (□+∂_t)u=0 in with (u,∂_tu)|_t=0=(u₀,u₁). Because the L² estimates and the L^∞ estimates of the solution u(t) are well known, in this paper we pay attention to the L^p estimates with 1p<2 (in particular, p=1) of the solution u(t) for t0. In order to derive L^p estimates we first give the representation formulas of the solution u(t)=∂_tS(t)u₀+S(t)(u₀+u₁) and then we directly estimate the exact solution S(t)g and its derivative ∂_tS(t)g of the dissipative wave equation with the initial data (u₀,u₁)=(0,g). In particular, when p=1 and n1, we get the L¹ estimate: u(t)_L¹Ce^−t/4(u_0W^n,1+u_1W^n−1,1)+C(u_0L¹+u_1L¹) for t0.     

Optimal location of the support of the control for the 1-D wave equation: numerical investigations

We consider in this paper the homogeneous 1-D wave equation defined on Ω⊂ℝ. Using the Hilbert Uniqueness Method, one may define, for each subset ω⊂Ω, the exact control v _ω of minimal L ²(ω×(0,T))-norm which drives to rest the system at a time T>0 large enough. We address the question of the optimal position of ω which minimizes the functional . We express the shape derivative of J as an integral on ∂ ω×(0,T) independently of any adjoint solution. This expression leads to a descent direction for J and permits to define a gradient algorithm efficiently initialized by the topological derivative associated with J. The numerical approximation of the problem is discussed and numerical experiments are presented in the framework of the level set approach. We also investigate the well-posedness of the problem by considering a relaxed formulation.     

Conditions for the Existence of Solutions of a Periodic Boundary-Value Problem for an Inhomogeneous Linear Hyperbolic Equation of the Second Order. I

We consider the periodic boundary-value problem u _tt − u _xx = g(x, t), u(0, t) = u(π, t) = 0, u(x, t + ω) = u(x, t). By representing a solution of this problem in the form u(x, t) = u ⁰(x, t) + ũ(x, t), where u ⁰(x, t) is a solution of the corresponding homogeneous problem and ũ(x, t) is the exact solution of the inhomogeneous equation such that ũ(x, t + ω) u x = ũ(x, t), we obtain conditions for the solvability of the inhomogeneous periodic boundary-value problem for certain values of the period ω. We show that the relation obtained for a solution includes known results established earlier. __________ Translated from Ukrains'kyi Matematychnyi Zhurnal, Vol. 57, No. 7, pp. 912–921, July, 2005.