共轭聚合物中均匀无序对极化子输运动力学的影响

基于扩展的Su-Schrieffer-Heeger紧束缚模型和非绝热动力学方法, 研究了共轭聚合物材料中均匀无序效应对极化子输运动力学的影响. 研究发现: 极化子的动力学输运过程由外加电场和均匀无序效应共同决定; 在大部分电场范围下, 均匀无序效应对极化子输运的影响不太明显, 几乎可以忽略; 但在弱电场下, 均匀无序效应不利于极化子输运. 与高斯型无序效应下极化子的输运过程相比, 具有均匀无序的薄膜形貌更有利于极化子输运.     

COMBINED EFFECTS OF SUBCOOLING AND SURFACE ORIENTATION ON POOL BOILING OF HFE-7100 FROM A SIMULATED ELECTRONIC CHIP

The effects of orientation and subcooling on pool boiling of the HFE-7100 dielectric liquid near atmospheric pressure (0.085 MPa) from a 10 × 10 mm smooth copper surface are investigated experimentally. Results are obtained for inclination angles θ = 0° (upward-facing), 30°, 60°, 90°, 120°, 150°, and 180° (downward-facing) and liquid subcoolings ΔT_sub = 0, 10, 20, and 30 K. Increasing θ decreases the saturation nucleate boiling heat flux at high surface superheats (ΔT_sat > 20 K), but increases it only slightly at lower surface superheats. The critical heat flux (CHF) decreases slowly with increasing θ from 0° to 90°, and then deceases faster with increasing θ to 180°. CHF increases linearly with increased subcooling, but the rate increases from 0.016 K^?1 at 0° to 0.048 K^?1 at 180°. At θ = 0° and ΔT_sub = 30 K, CHF is ～ 36 W/cm² and 24.45 W/cm² for saturation boiling, while at θ = 180° CHF = 10.85 W/cm² at ΔT_sub = 30 K and only 4.30 W/cm² at saturation. The developed correlation for CHF of HFE-7100, as a function of θ and ΔT_sub, is within ±10% of the present data. The recorded still photographs of the boiling surface in the experiments illustrate the effects of liquid subcooling and surface orientation at different nucleate boiling heat fluxes and surface superheats on vapor bubble accumulation and/or induced mixing at the surface.     

基于Supporting-Ellipsoid方法的自由曲面构造

为了在特定平面上获得任意形式的辐照分布,采用了Supporting-Ellipsoid设计方法来构造自由曲面反射镜。介绍了其设计思想和设计过程,并以具体的设计实例为例构建了自由曲面光学系统。仿真结果表明,在不计反射损失的情况下,系统效率达到了97%,较传统太阳模拟器光学系统提升了3倍以上,不均匀度达到5.26%,与理想状态有一定差距,这是因为设计中兼顾了计算时间和自由曲面光滑性所造成的。     

用能动光学技术控制激光焦线形态的方法研究与仿真计算

 用一块能动反射镜、一块柱面透镜和一块非球面透镜可组成新原理的焦线形态控制系统。随时改变能动反射镜形状以调制波面位相,能将入射激光束变换成幅照均匀、长度在一定范围内连续可调的焦线。针对高斯型入射光强,探讨了用该系统控制激光焦线形态的可行性。     

将混沌序列变换成均匀伪随机序列的普适算法

提出了一种将混沌序列变换成均匀伪随机序列的普适算法.这种算法基于计算机浮点数表示的bit位操作,不针对任何具体对象,可将任意连续或分段连续分布的实型随机变量转换成均匀分布的随机变量.理论分析表明,这种算法源于实型随机变量中普遍存在着的沿bit位以指数规律增强的均匀化趋势.任何实型的混沌序列,不论来自混沌映射系统还是混沌微分动力系统,都可以在同一个标准算法下变换成均匀分布的伪随机序列,因而是混沌伪随机数发生器标准化模块设计和硬件实现的关键技术基础. 关键词： 混沌 伪随机序列 均匀分布函数     

可变焦列阵柱面透镜均匀线聚焦系统

用两个列阵柱面透镜与非球面透镜组成变焦线聚焦系统，能将入射激光束会聚成辐照均匀、长度连续可调的焦线，它可用于Ｘ光激光实验研究．文中详细分析了焦线上光场分布的情况，给出了物理光学分析的结果，并与巳有技术作了比较．     

双通道共轴聚焦型X射线晶体光谱仪

研制了一种用于Z箍缩等离子体X射线光谱诊断的双通道共轴聚焦型晶体光谱仪。谱仪采用均匀色散(即线色散率为常数)和球面云母晶体作为两个通道的X射线色散元件,位于中轴线上的双胶片盒作为探测器,在大致相同的光谱范围内同时获取Z箍缩等离子体的时间积分光谱。在中国工程物理研究院"阳"加速器上开展了Z箍缩内爆摄谱实验,两通道分别获得了Z箍缩铝丝阵等离子体的类氢和类氦光谱谱线。实验结果表明:均匀色散通道光谱分布遵循均匀色散条件,实验得到的线色散率和设计值吻合很好,最大相对误差仅为3.48%,和球面晶体通道相比,它能更容易、更准确识别和处理光谱,在识别和分析陌生复杂光谱成分时具有优势。     

紫外LED圆环阵列均匀照明的实现方法

为构造指纹荧光检测中所需的均匀照明紫外光源,选择紫外LED阵列照明。采用光电探测器检测单颗LED的辐射角分布,拟合单个LED角分布函数;用8颗LED均匀置于半径为10 mm的圆环上,在圆环上方5 mm处的中心轴上放置一个LED;在给定的观察屏上照度不均匀误差下,根据斯派罗法则,确定观测屏与圆环阵列之间的距离,从而实现LED圆环阵列的照度分布均匀化。也可以给定观测屏到圆环的距离,确定轴上LED放置点到圆环的距离。实验结果表明,观测屏到圆环距离为11.0 cm时,在半径为10.0 mm的圆域内,照度不均匀相对误差小于1.27%。     

带状电子束的空间电荷场

 利用理论分析和数值计算的方法研究了矩形波导内均匀电流密度的带状电子束模型的空间电荷场,给出了该带状电子束模型的空间电荷场的解析表达式,并研究了空间电荷场随带状电子束的几何参数和物理参数的变化规律。研究表明：在不改变电流密度的前提下,更宽的电子束可以传输更强的束流,而空间电荷场并不随束宽度的增大而增大,但是增加电子束厚度会使空间电荷场显著增强,从而不利于高流强电子束的传输;对于相同电流的带状电子束,保持电子束厚度不变,增大电子束宽度,相应地降低电流密度是降低空间电荷场的一个很好的途径,而保持电子束的宽度不变,增大束厚度,相应地降低电流密度只会使沿着电子束截面宽度方向的电场减小,而沿着电子束截面厚度方向的电场基本不变;对于相同电流和电流密度的带状电子束,更宽、更薄的电子束横截面尺寸能使沿着电子束截面宽度方向的电场降到更低,而沿着电子束截面厚度方向的电场只是略有减小。     

均匀磁场对海森堡XX链中两体热纠缠的影响

通过计算比特数n不大于6海森堡XX链中的两体纠缠,发现只有当n为奇数时,最近邻纠缠在磁场为零时才出现下凹现象.当n为4或6时,非最近邻纠缠在磁场两边对称;当n为5时,非最近邻纠缠在磁场两边则不对称.     

均匀平面波圆孔衍射远场二阶矩问题

 研究了均匀平面波圆孔衍射远场光斑强度二阶矩的计算问题， 数值模拟计算了强度二阶矩随边缘高空间频率分量截去的百分数而变化的情况。认为用M ²因子定义均匀平面波的光束质量原则上是有问题的，但在规定高空间频率分量截去百分数的条件下，也是可以执行的。而在光束空间参数测量中，这种高空间频率分量的截去是一定会发生的。     

对铁磁质在非均匀磁场中受力的一点说明

对铁磁质在非均匀磁场中受力的两个公式之间的关系进行了说明,将珀塞尔和赵凯华在其各自《电磁学》教材中的观点统一起来.     

均质多边形薄板绕任一对角线转动的转动惯量

运用均质三角形薄板对任一边、对过顶点且与对边平行的轴的转动惯量公式,得到了用薄板的质量、边长及对角线长表示的均质多边形薄板对任一对角线的转动惯量.     

一类具有Markov性质的混沌系统的构造

本文构造了一类具有Markov性质的分段扩张线性映射, 计算表明其具有正的李雅普诺夫指数. 通过理论分析, 证明了其极限分布是均匀分布, 并给出了其最小周期的计算公式. 通过分析符号熵测度应用于此系统时的具体涵义, 指出该系统的复杂度与系统的最小周期之间存在着矛盾关系, 说明了此系统具有可控的复杂度并给出了其复杂度随系统参数变化时的理论极限公式. 通过统计测试和复杂度测试表明, 此系统产生的混沌序列服从均匀分布, 而通过参数的调整该系统的符号熵可以接近其理论极限, 而与Logistic映射和斜帐篷映射的基于近似熵和符号熵的对比实验可知, 本文所提系统具有更高的复杂度, 并有更长的最小周期. 这表明此系统比较适合用于构造保密通信系统. 关键词： 混沌 Markov性质 复杂度 均匀分布     

激光主动照明光学系统设计

为提高跟踪测量系统对暗弱目标的探测能力,设计一套自动化激光主动照明光学系统,对跟踪测量视场范围进行主动辅助照明。该系统在0.2~5 km距离处的照明直径均为10 m,计算出其在-20℃及+45℃的温度调焦量,照明仿真结果表明系统照明不均匀性15%。通过研究系统像差对照明均匀性的影响,以及对设计的调光组进行分析,得到调光组移动量与照明距离之间的理论关系,表明自动调节调光组位置即可实现不同照明距离处的均匀照明。设计和分析结果表明,该主动照明系统能够自动调节调光组位置,实现跟踪测量视场内的均匀照明,有利于跟踪测量系统对于暗弱目标的探测。     

Whether the Support Region of Three-Bit Uniform Quantizer Has a Strong Impact on Post-Training Quantization for MNIST Dataset?

Driven by the need for the compression of weights in neural networks (NNs), which is especially beneficial for edge devices with a constrained resource, and by the need to utilize the simplest possible quantization model, in this paper, we study the performance of three-bit post-training uniform quantization. The goal is to put various choices of the key parameter of the quantizer in question (support region threshold) in one place and provide a detailed overview of this choice’s impact on the performance of post-training quantization for the MNIST dataset. Specifically, we analyze whether it is possible to preserve the accuracy of the two NN models (MLP and CNN) to a great extent with the very simple three-bit uniform quantizer, regardless of the choice of the key parameter. Moreover, our goal is to answer the question of whether it is of the utmost importance in post-training three-bit uniform quantization, as it is in quantization, to determine the optimal support region threshold value of the quantizer to achieve some predefined accuracy of the quantized neural network (QNN). The results show that the choice of the support region threshold value of the three-bit uniform quantizer does not have such a strong impact on the accuracy of the QNNs, which is not the case with two-bit uniform post-training quantization, when applied in MLP for the same classification task. Accordingly, one can anticipate that due to this special property, the post-training quantization model in question can be greatly exploited.     

A universal algorithm to generate pseudo-random numbers based on uniform mapping as homeomorphism

A specific uniform map is constructed as a homeomorphism mapping chaotic time series into [0,1] to obtain sequences of standard uniform distribution. With the uniform map, a chaotic orbit and a sequence orbit obtained are topologically equivalent to each other so the map can preserve the most dynamic properties of chaotic systems such as permutation entropy. Based on the uniform map, a universal algorithm to generate pseudo random numbers is proposed and the pseudo random series is tested to follow the standard 0-1 random distribution both theoretically and experimentally. The algorithm is not complex, which does not impose high requirement on computer hard ware and thus computation speed is fast. The method not only extends the parameter spaces but also avoids the drawback of small function space caused by constraints on chaotic maps used to generate pseudo random numbers. The algorithm can be applied to any chaotic system and can produce pseudo random sequence of high quality, thus can be a good universal pseudo random number generator.     

Uniform Cantor Singular Continuous Spectrum for Nonprimitive Schrödinger Operators

It is shown that some Schrödinger operators, with nonprimitive substitution potentials, have pure singular continuous Cantor spectrum with null Lebesgue measure for all elements in the respective hulls.     

Revision of single atom local density and capture number varying with coverage in uniform depletion approximation and its effect on coalescence and number of stable clusters

In vapour deposition,single atoms (adatoms) on the substrate surface are the main source of growth.The change in its density plays a decisive role in the growth of thin films and quantum size islands.In the nucleation and cluster coalescence stages of vapour deposition,the growth of stable clusters occurs on the substrate surface covered by stable clusters.Nucleation occurs in the non-covered part,while the total area covered by stable clusters on the substrate surface will gradually increase.Carefully taking into account the coverage effect,a revised single atom density rate equation is given for the famous and widely used thin-film rate equation theory,but the work of solving the revised equation has not been done.In this paper,we solve the equation and obtain the single-atom density and capture number by using a uniform depletion approximation.We determine that the single atom density is much lower than that evaluated from the single atom density rate equation in the traditional rate equation theory when the stable cluster coverage fraction is large,and it goes down very fast with an increase in the coverage fraction.The revised equation gives a higher value for the ’average’ capture number than the present equation.It also increases with increasing coverage.That makes the preparation of single crystalline thin film materials difficult and the size control of quantum size islands complicated.We also discuss the effect of the revision on coalescence and the number of stable clusters in vapour deposition.     

An Image Array System for Uniform Illumination of Laser Fusion Target

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