约瑟夫森效应的一种初等阐述

用初等方法导出了约瑟夫森公式，阐述了约瑟夫森效应及其简单应用．     

平面静电场的试探法和复变函数法

本文中给出了平面静电场的两种简捷解法，即试探法和复变函数法．     

脉冲梯度场增强的DQF-COSY实验t1噪声研究

脉冲相位的不稳定性是导致二维谱中的t₁噪声的原因之一.本文从理论上和实验上对脉冲相位不稳定性所引起的t₁噪声进行了研究.从角动量算符I_x,I_y和I_z推导中发现,由于磁化矢量在P型和N型DQF-COSY实验的脉冲梯度场中进动方向的内在差异,一部分脉冲相位误差在P型DQF-COSY实验会被重聚掉,在N型DQF-COSY实验中却会被加重.因此P型DQF-COSY实验的t₁噪声比N型小.理论推导还得到t₁噪声在P型和N型中的理论比值为√3:√11.以上理论结果得到我们实验结果的支持.     

非线性延时修正光纤孤子方程的稳态解问题Ⅱ.漂移型扭结孤波解

利用一种与Ｂｃｈｌｕｎｄ变换有关的方法严格求含非线性延时项光孤立子方程,得到了该方程的漂移型扭结孤波解,并讨论了解的极限性质和相关物理问题。最后指出了该方程在γ＝０处的参数不稳定性问题     

The comparable structural,elastic anisotropic and thermophysical properties of advanced U–Si fuel to baseline UO2: a DTF method

The European Physical Journal B - Molecular dynamics and Monte Carlo methods are common measurements to study the diffusion coefficients of the fluid particles under restricted conditions. Here,...     

Euler calculations with embedded Cartesian grids and small-perturbation boundary conditions

This study examines the use of stationary Cartesian mesh for steady and unsteady flow computations. The surface boundary conditions are imposed by reflected points. A cloud of nodes in the vicinity of the surface is used to get a weighted average of the flow properties via a gridless least-squares technique. If the displacement of the moving surface from the original position is typically small, a small-perturbation boundary condition method can be used. To ensure computational efficiency, multigrid solution is made via a framework of embedded grids for local grid refinement. Computations of airfoil wing and wing-body test cases show the practical usefulness of the embedded Cartesian grids with the small-perturbation boundary conditions approach.     

利用电化学微分质谱在燃料电池的阴极研究碳载体的氧化

利用电化学微分质谱,在双薄层流动电解池中,通过检测二氧化碳产物的信号研究氧气与铂纳米粒子对碳载体氧化机理与动力学的影响．研究发现,碳载体可以在不同的电位区间内被氧化;氧气可以加速碳的氧化,在相同的电位下碳氧化生成二氧化碳产物的速率在氧气饱和溶液中是在氮气饱和溶液中的两倍;铂纳米粒子可以催化碳的氧化,在碳电极上,担载的铂纳米粒子可以大大降低碳氧化的过电势．讨论了铂与氧气促进碳氧化的机理．     

Preparation via solid-state reaction at room temperature and characterization of layered nanocrystalline NH4MnPO4·H2O

The layered nanocrystalline NH₄MnPO₄·H₂O was obtained by grinding MnSO₄·H₂O and (NH₄)₃PO₄·3H₂O in the presence of surfactant PEG-400 via a solid-state reaction at room temperature, maintaining the mixture at room temperature for 12 h, washing the mixture with water, and drying at 60 °C. The resulting NH₄MnPO₄·H₂O and its products of thermal decomposition were characterized using thermogravimetry and differential thermal analyses (TG/DTA), IR, X-ray powder diffraction (XRD), scanning electron microscopy (SEM), UV–vis, and magnetic susceptibility. The data showed that when dried at 60 °C for 5 h, highly crystallized orthorhombic NH₄MnPO₄·H₂O (space group Pmnm(59)) was obtained with an average particle size of 45 nm and an average interlayer distance of 0.8701 nm. On the other hand, monoclinic nanocrystalline Mn₂P₂O₇ with space group C2/m(12) was obtained when the product was calcined at 600 °C for 3 h. Magnetic susceptibility measurements from room temperature to 2.5 K point to ferrimagnetic ordering at T_N～17 K.     

Entropy squeezing of an atom with a k-photon in the Jaynes--Cummings model

The entropy squeezing of an atom with a k-photon in the Jaynes-Cummings model is investigated. For comparison, we also study the corresponding variance squeezing and atomic inversion. Analytical results show that entropy squeezing is preferable to variance squeezing for zero atomic inversion. Moreover, for initial conditions of the system the relation between squeezing and photon transition number is also discussed. This provides a theoretical approach to finding out the optimal entropy squeezing.     

A three-step system calibration procedure with error compensation for 3D shape measurement

System calibration, which usually involves complicated and time-consuming procedures, is crucial for any three-dimensional （3D） shape measurement system based on vision. A novel improved method is proposed for accurate calibration of such a measurement system. The system accuracy is improved with considering the nonlinear measurement error created by the difference between the system model and real measurement environment. We use Levenberg-Marquardt optimization algorithm to compensate the error and get a good result. The improved method has a 50% improvement of re-projection accuracy compared with our previous method. The measurement accuracy is maintained well within 1.5% of the overall measurement depth range.