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1.
定向背光柱透镜光栅式多视点自由立体显示器的串扰和亮度均匀性问题是影响其广泛应用的主要因素之一.本文通过分析串扰产生的原因,根据偏轴光线的成像光学原理,推导出液晶显示屏光开关板列单元与柱透镜组成的偏轴光学系统的参数计算式.提出一种液晶显示屏光开关蝶形单元结构,设计了采用该蝶形单元的定向背光自由立体显示背光源模组.模拟仿真结果表明:所设计的定向背光自由立体显示背光源可消除自由立体显示的串扰;在视点平面90%观看区域的串扰度小于0.5%,光束10%峰值宽度的串扰面积比γ=0,光束90%峰值宽度比普通液晶单元结构的增大37%,改善了不同位置观看图像亮度变化大的问题.  相似文献   

2.
虞家琪 《发光学报》1984,5(2):97-108
晶体场中能级分裂的计算--行列式波函数方法(4-1)用微扰法计算晶体场中能级分裂的示例 用简并微扰法计算晶体场中自由离子能级的分裂时,晶体场哈密顿量作为微扰,自由离子波函数为基,求出矩阵元,解久期方程,求出一级能量修正值即晶体场中能级的分裂,同时可求出自由离子基函数的线性组合作为零级近似波函数.下面以3d1组态的能级为例.  相似文献   

3.
多视点自由立体显示串扰分析与视区仿真   总被引:1,自引:0,他引:1  
侯春萍  许国  沈丽丽 《光子学报》2014,43(5):512001
对多视点自由立体显示的串扰成因进行了分析,推导出了无串扰观看点与光栅参数之间的关系;然后分别对垂直于显示器方向和平行于显示器方向的串扰进行了分析与计算,得到了屏前三维空间的串扰分布情况.仿真结果表明,沿显示屏幕垂直方向的视区范围大于水平方向的视区范围,而且在水平平行于屏幕的方向上,每一个视点存在多个理论无串扰观测点,但在垂直于屏幕方向上,每个视点只存在一个理论无串扰观测点.最后通过对屏前三维区域视点光强进行仿真,进一步验证了串扰计算的准确性,为自由立体显示系统的最佳设计与具体实现奠定了仿真基础.  相似文献   

4.
利用TracePro仿真软件对狭缝光栅自由立体LED显示器件的串扰进行仿真。首先,通过对狭缝光栅的设计原理分析,并基于LED模块的发光像素面积2 mm×2 mm,黑矩阵的面积1 mm×1 mm,设定最佳观看距离为5 m的两视点狭缝光栅自由立体LED显示器件,计算出光栅的狭缝宽度和挡光宽度都为2.87 mm。其次,利用这些参数,通过TracePro软件建立狭缝光栅自由立体LED显示器件的仿真模型,通过仿真运算得到左、右视频的光照度分布图,并通过归一化发现它们的光照度均匀性较差,观看时会导致"眩晕"现象。最后,借助自由立体显示器件串扰的测量方法,根据仿真左、右视频照度分布图的交叉曲线,定性分析了仿真结果,并结合Orign 9.1软件定量对仿真的串扰值进行计算,得出其串扰值为42.4%。这为进一步优化狭缝光栅自由立体LED显示器件的设计和性能提供了理论依据和技术支持。  相似文献   

5.
设计了一种用于裸眼3D显示屏的低串扰新型双面柱透镜光栅板,光栅板的入射面为等间距排列的与显示器子像素数量相同的凹形自由曲面光栅结构,出射面为斜置的凸形自由曲面光栅结构.根据裸眼3D显示原理和几何光学原理推导了双面光栅板的光栅单元自由曲面设计公式和光栅参数计算公式.通过MATLAB编程计算和SolidWorks软件建模得到光栅板模型.用TracePro软件对所设计的光栅板模型进行光线追迹仿真,结果表明:参数优化后的6视点斜置柱透镜双面光栅3D显示在最佳视角的图像串扰度为0.068%,与传统6视点斜置柱透镜光栅的最佳视角图像串扰度相比降低了2个数量级,并且在观看距离2 000mm~3 000mm范围内图像串扰度基本不变.  相似文献   

6.
利用费米子变换方法,将 Ising 自旋(S=1/2)反铁磁超晶格体系变换为粒子数不守恒的费米子体系.再利用量子统计微扰方法,在二级微扰近似下对周期为L=L_a+L_b(L_a=L_b)的 Ising 自旋(S=1/2)反铁磁超晶格进行了计算,求得了这种超晶格体系的自由能等一些热力学量和温度(T)、周期 L 的关系式.  相似文献   

7.
吴丹迪 《中国物理 C》1992,16(2):183-186
自由Dirac方程正、负宇称电子解的简并性可造成计算一级微扰能量的不确定性.以纯宇称解作为微扰场论的零级波函数虽然直接,但缺乏有力的理论根据.选择零级电子波函数的任意性是推导泡利方程和做Foldy-Wouthuysen变换不确定性的根源.  相似文献   

8.
徐开文  郭汉英 《物理学报》1989,38(12):2008-2018
在Krichever-Novikov(简称KN)弦的BRST量子化的基础上,采用Siegel的方法构造了任意给定亏格的KN弦的拟自由场论,并提出了一种非微扰拟自由弦场论的尝试。 关键词:  相似文献   

9.
本文利用复合粒子量子场论的微扰展开方法计算了双例外原子(π~±μ~?)的四体衰变的几率,并与自由μ衰变作了比较。  相似文献   

10.
王勤  赵悟翔  邹翠明 《光学技术》2019,45(5):617-621
针对观看自由立体显示器存在人眼焦点调节和集合不一致的根本生理问题,及观看时间稍长将引起立体观看视疲劳,甚至危害视觉健康的问题。提出了一种对自由立体显示器视疲劳程度进行预测的方法,由三个不同的立体观看视疲劳参数——视差值、视频帧率和串扰度组合得到27段立体测试视频,让观看者观看这些视频得到主观评价数据,采用多元线性回归的统计方法处理评价数据确定了自由立体显示器视疲劳的多元线性回归模型,并根据此模型对待评估立体视频的视疲劳程度进行有效预测。这种方法避免了反复的主客观评价对视觉系统的危害,减少主客观评价信息收集的复杂性。最重要的是,该模型能快速预测自由立体显示器视疲劳程度。  相似文献   

11.
The van Laar equation for the uniform substance phase is analyzed. Based on this, an expression for free energy is found. The structure of the expression allowed us to create a method for determining the free energy in an arbitrary order of the perturbation theory. A generalized equation for free energy is derived based on the using thermodynamic perturbation theory and the accelerated method of convergence of the series of the perturbation theory. This expression agrees well with the asymptotic behavior of the free energy and with the known experimental data. It can be successfully used to describe the behavior of the substance in a super-critical region, as well as to investigate the metastable phase. It is shown that the expression for free energy can be used for a broad class of substances.  相似文献   

12.
YAN Jun 《理论物理通讯》2007,48(4):653-656
The free energy at low temperature in 1D sine-Gordon-Thirring model with impurity coupling is studied by means of functional integrals method. For massive free sine-Gordon-Thirring model, free energy is obtained from perturbation expansion of functional determinant. Moreover, the free energy of massive model is calculated by use of an auxiliary Bose field method.  相似文献   

13.
The weak-coupling expansion for thermodynamic quantities in thermal field theories is poorly convergent unless the coupling constant is tiny.We discuss the calculation of the free energy for a hot gas of electrons and photons to three-loop order using hard-thermal-loop perturbation theory (HTLpt).We show that the hard-thermal-loop perturbation reorganization improves the convergence of the successive approximations to the QED free energy at large coupling,e ~ 2.The reorganization is gauge invariant by construction,and due to the cancellations among various contributions,we obtain a completely analytic result for the resummed thermodynamic potential at three loops.  相似文献   

14.
结合描述硬球固体Helmholtz自由能的自由体积方法与描述硬球固体径向分布函数的拟合的分析表达式与一阶热力学摄动理论,用于描述Lennard Jones(LJ)固体的Helmholtz自由能.按照一个修正的WCA方法将LJ势分为短程排斥部分与长程吸引部分,将文献中一个用于求取液相的等价的硬球直径的简单的迭代法扩展到固相,用于求取固相的等价的硬球直径.在固体Helmholtz自由能的计算中,使用200壳层,以便获得精确的结果.体相LJ液体的热力学特性由一个最近提出的状态方程求取.该方法很好地描述了LJ固体的过量Helmholtz自由能与状态方程,满意地描述了Lennard Jones模型的相平衡;通过选取合适的LJ势参数,能很好地描述了真实分子的融化曲线.  相似文献   

15.
A perturbation theory for square-well chain fluids is developed within the scheme of the (generalised) Wertheim thermodynamic perturbation theory. The theory is based on the Pavlyukhin parametrisations [Y. T. Pavlyukhin, J. Struct. Chem. 53, 476 (2012)] of their simulation data for the first four perturbation terms in the high temperature expansion of the Helmholtz free energy of square-well monomer fluids combined with a second-order perturbation theory for the contact value of the radial distribution function of the square-well monomer fluid that enters into bonding contribution. To obtain the latter perturbation terms, we have performed computer simulations in the hard-sphere reference system. The importance of the perturbation terms beyond the second-order one for the monomer fluid and of the approximations of different orders in the bonding contribution for the chain fluids in the predicted equation of state, excess energy and liquid–vapour coexistence densities is analysed.  相似文献   

16.
The mean spherical approximation is shown to be derivable from a perturbation expansion where the reference system follows the Percur-Yevick approximation. Then the MSA may be interpreted as a first-order expansion in which the perturbation is averaged with respect to the low-density reference distribution function. This represents a generalization of an equivalent interpretation previously made with respect to the free energy of a polar fluid.  相似文献   

17.
J P Sinha  S K Sinha 《Pramana》1990,35(5):473-483
The Barker-Henderson perturbation theory is used for a ν-dimensional fluid with square-well potential. Analytic expressions are given for the equation of state, excess free energy per particle and internal energy. The numerical results are discussed. A significant feature is the increase of the thermodynamic properties with increasing dimensionality.  相似文献   

18.
A free energy density functional theory (DFT) for nonuniform polymeric mixtures is proposed based on first order thermodynamic perturbation theory. The segment-density based free energy functional provides an accuracy comparable to the numerically intensive polymeric DFTs while preserving the computational simplicity of an atomic DFT. The presented applications for solutions and blends of branched and linear polymers demonstrate the capability of the theory to capture the entropic and enthalpic effects governing the microstructure.  相似文献   

19.
A perturbation series for the free energy of independent electrons is presented and applied to the problem of dia- and paramagnetism of the free electron gas. By using a periodic magnetic field the boundary conditions can be exactly satisfied. The results agree with those of other authors using approximate boundary conditions.  相似文献   

20.
ABSTRACT

The free energy of the square-well (SW) fluid is a quantity of great interest in thermodynamics and statistical mechanics. Several authors have calculated by simulations the first four terms in the high-temperature perturbation expansion for SW ranges from λ = 1 up to λ = 2.5 or 3. Besides, the asymptotic form of the first two terms in the expansion, for λ large, is known analytically. The information gathered so far seems to indicate that a range of λ = 3 is not far from this asymptotic van der Waals regime. In this work, we use the technique of singular value decomposition (SVD) to provide us with expressions of the SW free energy valid for all ranges of 1 ≤ λ and, for the higher-order terms, covering the density range upto the random close-packed state. Besides rendering unified expressions of the free energy for all ranges, the SVD allows us to separate the perturbation terms into a sum of products of functions of density and range, so that one can discern the most important contributions and extract the underlying density and range profiles.  相似文献   

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