振荡器链的非成对交联

本文考虑振荡链的非成对交联，包括单向交联和非成对双向交联，给出了锁相解的存在定理，并对其解的渐近性质作了分析。最后，用数值例子对非成对交联和成对交联作了一些比较分析。     

交联聚乙烯的结构形态与空间电荷分布

通过压力波法测量了交联聚乙烯中空间电荷的形成, 并对形成稳定空间电荷分布的交联聚乙烯样品用切片法测量了其表面电位, 用红外吸收光谱法对空间电荷的积累与结构形态相互作用的关系进行了研究.     

成批到达的有特殊服务时间的多重休假排队系统分析

本文利用嵌入马尔可夫链方法研究了多重休假M^X／Gn／1排队系统。首先，利用概率分析法得到了排队系统的嵌入马尔可夫链的一步转移概率矩阵，以此为依据得到系统的稳态队长和同批第一个接受服务顾客的稳态等待时间。     

多探头交联电缆绝缘层同轴度显示仪数据的统计分析与在线质量控制系统*

本文介绍了用于多探头交联电缆绝缘层同轴度显示仪数据的统计分析与在线质量控制系统, 实践表明文中所给出的离散曲率法是一种稳定、精确、计算时间更短的统计与几何相结合的变点搜索方法, 使用上明显优于SIC、似然比和Bayes等方法.     

一般随机环境中马氏链的强大数律

本文研究了具有离散参数的一般环境中马氏链的强大数定律.利用随机环境中马氏链停时,获得了加在绕积马氏链样本函数上大数定律成立的充分条件.     

双无限环境中马氏链的强极限定理

在双无限环境中马氏链的过程矩满足一定的条件下,通过停时和鞅收敛定理,得到双无限环境中马氏链的一类强极限定理.     

生物聚合物交联网络的力学响应

生物聚合物交联网络(crosslinked biopolymer networks)是由肌动蛋白微丝等生物纤维相互交联形成的复杂网络结构,它广泛存在于细胞骨架和生物凝胶等系统中,对维持细胞完整性、使细胞具有主动变形和抵抗被动变形能力起着不可或缺的作用,其力学响应及工作机理对细胞工程、组织工程的发展非常重要.生物聚合物交联网络中交联蛋白的结合能量通常较低,其解离和重连过程容易受到网络结构变形和环境热涨落等因素的影响.实验中发现生物聚合物交联网络在小变形时刚度较低,但随着变形的增加,网络整体刚度会呈现数量级的增加,如果变形继续增加并超过一定阈值,网络刚度将急剧下降,这种应变硬化到软化的现象引起了研究者的广泛关注.已有理论模型和数值模拟发现,生物聚合物交联网络的硬化主要来源于纤维变形模式从弯曲到拉伸的转化,而软化则是由于网络中交联蛋白解离导致结构弱化和应力松弛.从生物聚合物交联网络的微观组成和结构出发,综述了生物聚合物纤维的力学模型、交联蛋白的力学属性和交联方式、交联网络的主要构型以及测量网络力学响应的实验方法,重点讨论了理论建模、有限元模拟、分子动力学等方法在研究生物聚合物交联网络非线性力学行为的进展,旨在为具有不同专业背景的研究者了解并开展生物聚合物交联网络力学响应的相关研究提供参考,也有助于机理化、定量化地理解细胞骨架中蕴含的结构-功能关系.     

微波晶体管振荡器设计的最优化方法

本文在分析微波振荡器电路特性的基础上，建立了精确、可靠的数学模型，编写出最优化设计程序，从而提高了微波振荡器电路设计的效率和精度。     

高校应用数学学报第15卷(2000年)B辑(英文版)第4期目次和提要

无环多重图的最大亏格的下界李德明 (首都师大数学系 )　刘彦佩 (北方交通大学数学系 )依照无环多重图的连通度 ,得到了它们的最大亏格的下界 .这不仅回答了 Chen,Archdeacon和 Gross的问题 ,也推广了现有结果 .这样 ,无环多重图的最大亏格的下界问题便有了完满的结论 .3 -连通无环多重图的最大亏格的紧下界李德明 (首都师大数学系 )　刘彦佩 (北方交通大学数学系 )证明了如果圈秩大于等于 1 0 ,3 -连通无环多重图的最大亏格至少是三分之一圈秩加一 ,有无限多个 3 -连通无环多重图的最大亏格取到这一下界 .具分段常变元的时滞微分方程的振…     

耦合型Mathieu方程及其粒子的共振穿越

本文用多重尺度法讨论了耦合型Mathieu方程解的稳定性及其它的一阶不稳定区,并分析了粒子穿越v_x+2v_z=N共振线的动力学行为,导出了工程要求的最小加速电压。     

Modulation of synchronization dynamics in a network of self-sustained systems

This paper addresses the combined modulatory effects of non-nearest neighbor oscillators and local injection on synchronized states dynamics with their corresponding stability boundaries in a network of self-sustained systems. The Whittaker method and Floquet theory are used to predict analytically the stability of these states for identical and non-identical coupling parameters. Charts revealing the modulation of synchronized states and their stability boundaries at the second order of interaction in the cases of identical and non-identical coupling parameters are constructed with and without an external signal locally injected in the network. Numerical simulations validate and complement the results of analytical surveys. The limits of the stability regions are numerically explored when a small amount of Gaussian white noise is also injected in the network.     

Asymptotic Localization of Energy in Nondisordered Oscillator Chains

We study two popular one‐dimensional chains of classical anharmonic oscillators: the rotor chain and a version of the discrete nonlinear Schrödinger chain. We assume that the interaction between neighboring oscillators, controlled by the parameter ? > 0, is small. We rigorously establish that the thermal conductivity of the chains has a nonperturbative origin with respect to the coupling constant ?, and we provide strong evidence that it decays faster than any power law in ? as ? → 0. The weak coupling regime also translates into a high‐temperature regime, suggesting that the conductivity vanishes faster than any power of the inverse temperature. To our knowledge, it is the first time that a clear connection has been established between KAM‐like phenomena and thermal conductivity. © 2015 Wiley Periodicals, Inc.     

Synchronization in nonlinear oscillators with conjugate coupling

In this work, we investigate the synchronization in oscillators with conjugate coupling in which oscillators interact via dissimilar variables. The synchronous dynamics and its stability are investigated theoretically and numerically. We find that the synchronous dynamics and its stability are dependent on both coupling scheme and the coupling constant. We also find that the synchronization may be independent of the number of oscillators. Numerical demonstrations with Lorenz oscillators are provided.     

Synchronization transition in degenerate optical parametric oscillators induced by nonlinear coupling

In this paper, the synchronization of certain degenerate optical parametric oscillators is investigated in detail. Complete and/or partial synchronization can be reached when linear controller, constructed by the real part or imaginary part of the subharmonic mode, is imposed on the chaotic degenerate optical parametric oscillators with appropriate coupling intensity. The Lyapunov exponents under different coupling coefficients are calculated to find the critical condition for complete synchronization. Transition from complete synchronization to partial synchronization is observed when nonlinear coupling is introduced into the two chaotic oscillators. It is found that synchronization of chaotic oscillators keeps robust when the intensity of the nonlinear coupling is less than the intensity of the linear coupling; the complete synchronization state is destructed and transient period for partial synchronization is in certain delay when the intensity of the nonlinear coupling is beyond the intensity of the linear coupling.     

The dynamics ofn weakly coupled identical oscillators

Summary We present a framework for analysing arbitrary networks of identical dissipative oscillators assuming weak coupling. Using the symmetry of the network, we find dynamically invariant regions in the phase space existing purely by virtue of their spatio-temporal symmetry (the temporal symmetry corresponds to phase shifts). We focus on arrays which are symmetric under all permutations of the oscillators (this arises with global coupling) and also on rings of oscillators with both directed and bidirectional coupling. For these examples, we classify all spatio-temporal symmetries, including limit cycle solutions such as in-phase oscillation and those involving phase shifts. We also show the existence of “submaximal” limit cycle solutions under generic conditions. The canonical invariant region of the phase space is defined and used to investigate the dynamics. We discuss how the limit cycles lose and gain stability, and how symmetry can give rise to structurally stable heteroclinic cycles, a phenomenon not generically found in systems without symmetry. We also investigate how certain types of coupling (including linear coupling between oscillators with symmetric waveforms) can give rise to degenerate behaviour, where the oscillators decouple into smaller groups.     

Dynamics of a ring network of phase-only oscillators

We investigate the existence, stability and bifurcation of phase-locked motions in a ring network consisting of phase-only oscillators arranged in multiple simple rings (sub-rings) which are themselves arranged in a single large ring. In the case of networks with three or four sub-rings, we give approximate expressions for critical coupling coefficients which must be exceeded in order for phase-locking to occur.     

Isotropy of Angular Frequencies and Weak Chimeras with Broken Symmetry

The notion of a weak chimeras provides a tractable definition for chimera states in networks of finitely many phase oscillators. Here, we generalize the definition of a weak chimera to a more general class of equivariant dynamical systems by characterizing solutions in terms of the isotropy of their angular frequency vector—for coupled phase oscillators the angular frequency vector is given by the average of the vector field along a trajectory. Symmetries of solutions automatically imply angular frequency synchronization. We show that the presence of such symmetries is not necessary by giving a result for the existence of weak chimeras without instantaneous or setwise symmetries for coupled phase oscillators. Moreover, we construct a coupling function that gives rise to chaotic weak chimeras without symmetry in weakly coupled populations of phase oscillators with generalized coupling.     

Universal occurrence of mixed-synchronization in counter-rotating nonlinear coupled oscillators

By coupling counter-rotating coupled nonlinear oscillators, we observe a “mixed” synchronization between the different dynamical variables of the same system. The phenomenon of amplitude death is also observed. Results for coupled systems with co-rotating coupled oscillators are also presented for a detailed comparison. Results for Landau–Stuart and Rössler oscillators are presented.