一类四阶两点边值问题多个正解的存在性

该文研究两端固定的弹性梁方程边值问题狔′′′′（狓）＝犳（狓，狔（狓）），　狓∈ （０，１），狔（０）＝狔（１）＝狔′（０）＝狔′（１）＝０多个正解的存在性．主要结果的证明基于锥上的不动点定理以及相应的线性问题的Ｇｒｅｅｎ函数的性质．     

半线性抛物方程可变号解的全局存在和爆破

该文研究了如下柯西问题狌狋＝狌狓狓＋ （狋＋１）－σ／２狘狓狘σ狘狌狘狆－１狘狌狘，　狓∈犚，狋∈犚＋ ，狌（狓，０）＝狌０（狓），　狓∈犚｛ ．其中参数σ≥０，狌０（狓）在犚上犽次变号，满足某种速降条件．证明了：如果ｍａｘ｛σ，１｝＜狆≤１＋２犽＋１，那么所有非零解在有限时间内爆破；如果狆＞ｍａｘ｛σ，１＋２犽＋１｝则存在一个非零全局解．     

相依样本下线性模型误差分布的相合估计

对于线性模型狔犻＝狓犻′β＋犲犻，犻＝１，…，狀，设误差序列｛犲犻｝是平稳的α 混合序列，犳（狓）为其 公共的未知密度函数，我们讨论了基于残差的犳（狓）的核估计＾犳狀（狓）＝１狀犪狀∑狀犻＝１犓（＾犲狀犻－狓犪狀）的弱相合性、逐点强相合性、一致强相合性及其收敛速度，其中＾犲狀犻为Ｌ．Ｓ．估计的残差．     

一个抛物型方程不适定问题的小波正则化方法

一维抛物型方程如下定解问题狌狋＋狌狓＝狌狓狓， ０≤狓＜ ∞，０≤狋＜ ∞，狌（１，狋）＝犵（狋）， ０≤狋＜ ∞，狌（狓，０）＝０， 狓≥０烅烄烆．是一个不适定问题．数据犵的微小变化可以引起解的巨大误差．该文通过构造一个在频域具紧支集的小波并在尺度空间上展开数据和解，滤除了高频分量，并结和Ｇａｌｅｒｋｉｎ方法，建立了一种逼近准确解的正则化方法，恢复了解对数据的连续依赖性，并建立了误差估计．     

超扩散过程的遍历定理

考虑初始测度为Ｌｅｂｅｓｇｕｅ测度μ 的一致椭圆超扩散过程，其分枝特征为ψ（狓，狕）＝犫（狓）狕＋γ（狓）狕２．该文研究这类超过程的占位时过程的极限性质．对系数犫（狓）及γ（狓）做必要的限制，得到了占位时过程在空间维数犱≤２的遍历定理，我们的结果是［６］的补充．     

中立型时滞微分方程的渐近稳定性

考虑具有正负系数的中立型时滞微分方程ｄｄ狋［狓（狋）－犘（狋）狓（狋－τ）］＋犙（狋）狓（狋－δ）－犚（狋）狓（狋－σ）＝０，　狋≥狋０， 其中Ｐ（ｔ）∈Ｃ（［ｔ０，∞），Ｒ），Ｑ（ｔ），Ｒ（ｔ）∈Ｃ（［ｔ０，∞），Ｒ＋ ），τ，δ，σ∈（０，∞）．获得了该方程零解 一致稳定及渐近稳定的充分条件，它推广并改进了现有文献中的结论．     

一簇Lorenz映射的混沌行为与统计稳定性

该文研究一簇Ｌｏｒｅｎｚ映射犛犪：［０,１］→［０,１］（０＜犪＜１）犛犪（狓）＝狓＋犪　狓∈ ［０,１－犪）｛（狓＋犪－１）／犪　狓∈ ［１－犪,１］．从拓扑的角度考虑了犛犪的混沌行为,证明了：犛犪有稠密轨道;犛犪的周期的集合犘犘（犛犪）＝｛１,犿＋１,犿＋２,…｝,其中犿为使犪犿＜１－犪成立的最小正整数;犛犪的拓扑熵犺（犛犪）＞０;几乎所有（关于Ｌｅｂｅｓｇｕｅ测度）的点狓的Ｌｙａｐｕｎｏｖ指数λ（犛犪,狓）＝λ犪＞０．从统计的角度讨论了犛犪的稳定性．我们用下界函数方法证明了犛犪是统计稳定的,并且狌犵犪（犃）＝∫犃犵犪（狓）ｄ狓（犃∈犅）为犛犪的唯一绝对连续（关于Ｌｅｂｅｓｇｕｅ测度）不变概率测度．同时,不变密度犵犪在参数扰动和随机作用的随机扰动下是稳定的．     

图的有特殊性质的k-因子和半k-因子

设犽≥１是一个整数,犌是一个２ 边连通图,犝是犞（犌）的子集．设犉是犌的支撑子图,使得对所有狓∈犞（犌）－犝,有ｄｅｇ犉（狓）＝犽,若对所有狓∈犝,有ｄｅｇ犉（狓）≥犽,则犉称为带缺损犝的上限半 犽 因子;若对所有狓∈犝,有ｄｅｇ犉（狓）≤犽,则犉称为带缺损犝的下限半 犽 因子．本文证明了若犽｜犞（犌）｜是偶数,｜犞（犌）｜≥犽＋２,对犞（犌）的任一基数为犽＋２的子集犝,如果对任意犲∈犈（犌）,犌都 有一个带缺损犝的上限半 犽 因子含犲,则犌是犽 覆盖的;若犽≥２是一个偶数,｜犞（犌）｜＞２犽＋４,对犞（犌）的任一基数为犽＋３的子集犝,如果对任意犲∈犈（犌）,犌有一个带缺损犝的上限半 犽 因子含犲,则犌是犽 覆盖的;还证明了若犽｜犞（犌）｜是偶数,｜犞（犌）｜≥犽＋４,对犞（犌）的任一基数为３的子集犝,如果对任意犲∈犈（犌）,犌都有一个带缺损犝的下限半 犽 因子含犲,则犌是犽 覆盖的．     

Kneser图的分数染色临界性

图犌的一个分数染色是从犌的独立集的集合ζ 到区间［０，１］的一个映射犆，使得对任意顶点狓，都有： Σ 犛∈ζ，ｓ．ｔ．狓∈狊犆（犛）１，我们将此分数染色的值定义为Σ犛∈ζ犮（犛）．图犌的分数色数χ犳（犌）是它的所有分数染色的值的下确界．给出了分数染色临界性的定义并讨论了Ｋｎｅｓｅｒ图的分数染色临界性．     

高阶奇异积分的小波逼近及数值计算

该文所讨论的是在Ｈａｄａｍａｒｄ主值意义下，高阶奇异积分（犛犳）（狋）＝∫ 犳（狓）（狓－狋）狀＋１ｄ狓，　　狀≥１的小波逼近及数值计算．特别是当小波函数未知时，借助于方程（３．１），对高阶奇异积分作数值计算，建立了收敛性定理．     

Research on traveling wave solutions for a class of (3+1)-dimensional nonlinear equation

Nonlinear wave phenomena are of great importance in the nature, and have became for a long time a challenging research topic for both pure and applied mathematicians. In this paper the solitary wave, kink (anti-kink) wave and periodic wave solutions for a class of (3+1)-dimensional nonlinear equation were obtained by some effective methods from the dynamical systems theory.     

Do peaked solitary water waves indeed exist?

Many models of shallow water waves, such as the famous Camassa–Holm equation, admit peaked solitary waves. However, it is an open question whether or not the widely accepted peaked solitary waves can be derived from the fully nonlinear wave equations. In this paper, a unified wave model (UWM) based on the symmetry and the fully nonlinear wave equations is put forward for progressive waves with permanent form in finite water depth. Different from traditional wave models, the flows described by the UWM are not necessarily irrotational at crest, so that it is more general. The unified wave model admits not only the traditional progressive waves with smooth crest, but also a new kind of solitary waves with peaked crest that include the famous peaked solitary waves given by the Camassa–Holm equation. Besides, it is proved that Kelvin’s theorem still holds everywhere for the newly found peaked solitary waves. Thus, the UWM unifies, for the first time, both of the traditional smooth waves and the peaked solitary waves. In other words, the peaked solitary waves are consistent with the traditional smooth ones. So, in the frame of inviscid fluid, the peaked solitary waves are as acceptable and reasonable as the traditional smooth ones. It is found that the peaked solitary waves have some unusual and unique characteristics. First of all, they have a peaked crest with a discontinuous vertical velocity at crest. Especially, unlike the traditional smooth waves that are dispersive with wave height, the phase speed of the peaked solitary waves has nothing to do with wave height, but depends (for a fixed wave height) on its decay length, i.e., the actual wavelength: in fact, the peaked solitary waves are dispersive with the actual wavelength when wave height is fixed. In addition, unlike traditional smooth waves whose kinetic energy decays exponentially from free surface to bottom, the kinetic energy of the peaked solitary waves either increases or almost keeps the same. All of these unusual properties show the novelty of the peaked solitary waves, although it is still an open question whether or not they are reasonable in physics if the viscosity of fluid and surface tension are considered.     

The bifurcation and exact travelling wave solutions for the modified Benjamin-Bona-Mahoney (mBBM) equation

By using methods from dynamical systems theory, this paper researches the bifurcation and exact travelling wave solutions for the modified Benjamin-Bona-Mahoney (mBBM) equation. Implicit exact parametric representations of all travelling wave solutions as well as some explicit analytic solutions are given. Specially, breaking wave solutions are obtained, which KdV equation does not include.     

Bifurcation of travelling wave solutions for （2＋1）-dimension nonlinear dispersive long wave equation

In this paper,the bifurcation of solitary,kink,anti-kink,and periodic waves for （2＋1）-dimension nonlinear dispersive long wave equation is studied by using the bifurcation theory of planar dynamical systems.Bifurcation parameter sets are shown,and under various parameter conditions,all exact explicit formulas of solitary travelling wave solutions and kink travelling wave solutions and periodic travelling wave solutions are listed.     

利用GM(1,1)模型预测曲线波形

针对给出的函数y=f(x),x∈[a,b],将其值域进行n等分,设yi为其中任一分点,对应x=xi(i=1,2,…,m),用GM(1,1)模型对序列{x1,x2,…,xm}进行预测,得到曲线y=f(x)在下一段时间与直线y=yi的交点位置.当GM(1,1)模型的误差较大时,可利用带有残差修正的GM(1,1)模型进行残差修正,以提高GM(1,1)模型预测值的精确度.     

A meshfree method for the numerical solution of the RLW equation

In this paper, we present a meshfree technique for the numerical solution of the regularized long wave (RLW) equation. This approach is based on a global collocation method using the radial basis functions (RBFs). Different kinds of RBFs are used for this purpose. Accuracy of the new method is tested in terms of _L2$L_2$ and _L∞$L_{\infty }$ error norms. In case of non-availability of the exact solution, performance of the new method is compared with existing methods. Stability analysis of the method is established. Propagation of single and double solitary waves, wave undulation, and conservation properties of mass, energy and momentum of the RLW equation are discussed.     

New multisoliton solutions of the (2+1)-dimensional dispersive long wave equations

IntroductionSoliton is a complicated mathematical structure based on the nonlinear evolution equation.(1+ 1)-dimensional soliton and solitary wave solutions have been studied we1l and widely appliedto many physics fields like the condense matter physics, fluid mechanics, plasma physics, optics,etc. However, to find some exact physically significant soliton solutions in (2+l)-dimensions ismuch more difficult than in (1+1)-dimensions. Recently, by using some different approashes,one special type…     

Bifurcations of travelling wave solutions for the generalized (2+1)-dimensional Boussinesq-Kadomtsev-Petviashvili equation

By using the bifurcation theory of dynamical systems, we study the generalized (2+1)-dimensional Boussinesq-Kadomtsev-Petviashvili equation, the existence of solitary wave solutions, compacton solutions, periodic cusp wave solutions and uncountably infinite many smooth periodic wave solutions are obtained. Under different parametric conditions, various sufficient conditions to guarantee the existence of the above solutions are given. Some exact explicit parametric representations of the above waves are determined.     

The backward group preserving scheme for multi-dimensional nonhomogeneous and nonlinear backward wave problems

In this study, we utilize a backward group preserving scheme (BGPS) to cope with the nonhomogeneous as well as nonlinear backward wave problems (BWPs). Because the solution does not continuously count on the given information, the BWP is well-known to be seriously ill-posed. When six numerical instances are examined, we reveal that the BGPS is capable of tackling the nonhomogeneous and nonlinear BWPs. Besides, the BGPS is also robust enough against the perturbation even with the boisterous final data, of which the numerical results are rather accurate, effective and stable.     

Construction of traveling wave solutions of the (2 + 1)-dimensional modified KdV-KP equation

Traveling wave solutions have played a vital role in demonstrating the wave character of nonlinear problems emerging in the field of mathematical sciences and engineering. To depict the nature of propagation of the nonlinear waves in nature, a range of nonlinear evolution equations has been proposed and investigated in the existing literature. In this article, solitary and traveling periodic wave solutions for the (2 + 1)-dimensional modified KdV-KP equation are derived by employing an ansatz method, named the enhanced (G′/G)-expansion method. For this continued equation, abundant solitary wave solutions and nonlinear periodic wave solutions, along with some free parameters, are obtained. We have derived the exact expressions for the solitary waves that arise in the continuum-modified KdV-KP model. We study the significance of parameters numerically that arise in the obtained solutions. These parameters play an important role in the physical structure and propagation directions of the wave that characterizes the wave pattern. We discuss the relation between velocity and parameters and illustrate them graphically. Our numerical analysis suggests that the taller solitons are narrower than shorter waves and can travel faster. In addition, graphical representations of some obtained solutions along with their contour plot and wave train profiles are presented. The speed, as well as the profile of these solitary waves, is highly sensitive to the free parameters. Our results establish that the continuum-modified KdV-KP system supports solitary waves having different shapes and speeds for different values of the parameters.