Uniformly continuous superposition operators in the space of bounded variation functions

Let I, J ? ? be intervals. The main result says that if a superposition operator H generated by a function of two variables h: I × J → ?, H (φ)(x) ? h (x, φ (x)), maps the set BV (I, J) of all bounded variation functions, φ: I → J into the Banach space BV (I, ?) and is uniformly continuous with respect to the BV ‐norm, then h (x, y) = a (x)y + b (x), x ∈ I, y ∈ J, for some a, b ∈ BV (I, ?) (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Accurate bending analysis of rectangular plates with two adjacent edges free and the others clamped or simply supported based on new symplectic approach

The symplectic geometry approach is introduced for accurate bending analysis of rectangular thin plates with two adjacent edges free and the others clamped or simply supported. The basic equations for rectangular plates are first transferred into Hamilton canonical equations. Using the symplectic approach, the analytic solution of rectangular thin plate with two adjacent edges simply supported and the others slidingly supported is derived. Accurate bending solutions of title problems are then obtained using the superposition method. The approach used in this paper eliminates the need to pre-determine the deformation function and is hence more reasonable than conventional methods. Numerical results are presented to demonstrate the validity and efficiency of the approach as compared with those reported in other literatures.     

A simple and effective scheme for data reduction of stress relaxation incorporating physical-aging effects: An analytical and numerical analysis

A simple methodology for obtaining viscoelastic parameters from the stress relaxation tests incorporating physical-aging effects is presented. The method assumes that the experimental data are in the linear viscoelastic domain. Three different mathematical representations of the viscoelastic stress relaxation modulus are analysed and used. Experimental data obtained from literature and simulated data with a random error are used to evaluate the proposed methodology. It is proved that it can capture very well the relaxation modulus of polymers irrespective of the mathematical representation used for the relaxation modulus. Moreover, the methodology proved to be reasonably insensitive to random noise. Extrapolation predictions were also evaluated for the proposed models with very good results.     

迭加态的量子统计特性

本文利用量子力学迭加原理,讨论了相干态与Fork态的迭加产生的压缩和反聚束效应.结果表明在一些迭加态中存在两个压缩区,两个压缩区之问的区域反聚束效应较强,压缩效应及反聚束效应的强弱与相干态的平均光子数|α|~2及Fork态|m>的光子数m密切相关.文章最后一节讨论了在实验室如何实现这一压缩迭加态.     

材料力学用叠加法求梁变形个别例题的商榷

在现行的某些材料力学教材中,用叠加法求梁变形一节的个别例题,其解题方法并不符合所在教材定义的叠加原理。我们认为,这些例题不利于学生掌握叠加原理,有可能在他们的头脑中形成关于这个原理的模糊概念。鉴于叠加原理是固体力学中比较重要的原理,因此,将此问题提出,以供广大教师及力学工作者探讨。     

驻波振幅分布研究

本文研究了入射波与经固定界面一次、二次及多次反射所生的反射波迭加而成的驻波的振幅分布规律，并得出了一些有意义的结果。     

无限大扇形板状油藏水平井不稳定压力公式的推导

利用GringaLrten提出的点源函数、镜像映射方法和叠加原理推导了无限大板状油藏中一口水平井的不稳定压力公式,并对无限大扇形板状油藏中的水平井进行了研究,给出了具有a(只要2π/a为整数)角的无限大扇形板状油藏中水平井的不稳定压力通式.该通式计算较方便,为断块油藏水平井的开采提供了理论依据.     

Influence of turbulence on the beam propagation factor of Gaussian Schell-model array beams

The analytical expression for the beam propagation factor (M²-factor) of Gaussian Schell-model (GSM) array beams propagating through atmospheric turbulence is derived. It is shown that the M²-factor of GSM array beams depends on the beam number, the relative beam separation distance, the beam coherence parameter, the type of beam superposition, and the strength of turbulence. The turbulence results in an increase of the M²-factor. However, for the superposition of the intensity the M²-factor is less sensitive to turbulence than that for the superposition of the cross-spectral density function. The M²-factor of GSM array beams is larger than that of the corresponding Gaussian array beams. However, the M²-factor of GSM array beams is less affected by turbulence than that of the corresponding Gaussian array beams. For the superposition of the cross-spectral density function a minimum of the M²-factor of GSM array beams may appear in turbulence, which is even smaller than that of the corresponding single GSM beams.     

单模单参数q光场叠加态的压缩及高阶压缩特性

本文构造了一种单模单参数q光场叠加态|Ψ>_q=c(|α>_q+β|0>_q),利用Zhang等人提出的单模辐射场的振幅M次方压缩的定义对态|Ψ>_q的压缩及高阶压缩特性进行了详细的研究.结果发现,在一定的条件下,态|Ψ>_q可存在任意的M次方压缩效应. 最后,通过数值计算还详细研究了态|Ψ>_q的压缩和平方压缩性质.     

第Ⅰ类两态叠加多模叠加态光场的非线性高阶压缩特性研究

本文在文献20的基础上进一步提出了多模辐射场的N-Y最小测不准态、N-H最小测不准态、N-Y压缩最小测不准态以及N-H压缩最小测不准态等的定义.构造了由多模(q模)相干态|{Z_j}>_q及其相反态|{-Z_j}>_q的线性叠加所组成的第Ⅰ类两态叠加多模叠加态光场|ψ₁⁽²⁾>_q,利用文献20新近提出的有关多模辐射场的两种非线性高阶压缩的定义,首次对态|ψ₁⁽²⁾>_q的N次方Y压缩及N次方H压缩效应进行了详细研究.结果表明,1)当N为偶数时,态|ψ₁⁽²⁾>_q恒处于N-Y最小测不准态;当N为奇数时,态|ψ₁⁽²⁾>_q在一定条件下可呈现出周期性变化的、任意阶的N次方Y压缩效应.2)当q·N为偶数时,态|ψ₁⁽²⁾>_q恒处于N-H最小测不准态;当q·N为奇数时,在另外的条件下,态|ψ₁⁽²⁾>_q则可呈现出周期性变化的、任意阶的N次方H压缩效应.3)N次方Y压缩及N次方H压缩效应的压缩深度与腔模总数q、压缩参数R_j以及压缩阶数N等非线性相关,后者与上述参量的非线性关联程度要比前者的更强.