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 Reflection and Refraction of the Planar Electromagnetic Wave on the Interface Between Two Media 平面电磁波在两种介质表面上的反射与折射 短句来源 By analysing synthesis wave of two symmetry uniform plane electromagnetic waves, we get TE electromagnetic wave in two plane conducting plates due to the continuous reflections between two plane conducting plates, and point out that the transmission direction of the energy of TE electromagnetic wave is the direction of waveguide length. 通过对两列对称于Z轴方向传播的均匀平面电磁波迭加后的合成电磁波的分析，得出在两块平行导板之间，由于两导板壁对平面电磁波连续反射结果形成了TE型电磁波，并指出TE型电磁波的能量是沿波导长度方向传播的。 短句来源 With the help of Ginzburg-Landau-Devonshire (GLD) theory, the influence of imperfect surface layers on the properties of first-order ferroelectric thin films intercalated between two metal electrodes is theoretically studied. 应用Ginzburg Landau Devonshire(GLD)理论研究了非理想表面对夹持在两个金属电极间的一级铁电薄膜性质的影响. 短句来源 The calculation results indicate that the wave packet distribution of the 61∑+ state and the wave packet transfer between two states can be controlled by altering the parameters of the laser pulses. 研究结果表明:通过改变激光参数可以控制波包在两个势阱中的分布以及在两态间的转移; 短句来源 Comparing with the NM/FI/FI/NM double spin filter junction, this kind of double spin filter tunnel junction is developed by inserting a new NI layer between two FI layers. The purpose of inserting new NI layer is to decrease the interlayer exchange coupling between two FI layers, which would have disadvantage effects on the TMR and sensitivity of the double spin filter junctions. 该磁性隧道结是在NM/FI/FI/NM型双自旋过滤磁隧道结的基础上,进一步在两个FI层之间插入一NI层,以期克服由于两个FI层紧密靠在一起,界面处两层FI间的磁矩可能存在很强的交换耦合作用导致TMR下降并影响双自旋过滤隧道结的灵敏度的缺点。 短句来源 更多
 两相邻
 The liquid crystal director distribution in LCoS is simply calculated, and the picture of LC director structure between two adjacent display pixels inside the cell is given. The spacing grid is 50×50×20, the solving time is 564.36 s by the computer of Pentium 4, 2.8 GHz. 文章最后基于此方法针对LCoS中指向矢的分布进行了简单的模拟,给出了两相邻显示像素的指向矢分布图形,网格划分为50×50×20个节点,在Pentium4,2.8GHz的计算机上求解需564.36s。 短句来源 Actone molecular sited in the tube between two resorcinarenes. 中性分子丙酮寄宿于管道中两相邻间杯芳烃之间。 短句来源 By using a fiber to delay the pulse light of CuBr laser, velocity of light can be obtained with geometry length of fiber and time interval between two light pulses. 利用光纤对溴化亚铜激光器输出的脉冲激光进行延时,通过常规测长手段测得光纤的几何长度并用示波器测出两相邻光脉冲间的时间间隔,即可获得光速. 短句来源 Continuously varying the trap frequency between two neighboring points of the denumerable infinite set, from the quantum perturbation technique we find the energy-band structure based on the exact discrete spectra in which the bands are narrower and the gaps wider. 在该点集内两相邻点之间连续变化阱频,由量子微扰法得到以精确分立谱为基础的能带结构,包括较宽的能隙和较窄的带宽. 短句来源

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 between two
 Extending this theory, we show how to use correlations between two processes to predict one from the other. Extending this theory, we show how to use correlations between two processes to predict one from the other. It introduces notions of localization and approximation between two frames ${\frak F} = \{f_i\}_{i\in I}$ and ${\frak E} = \{e_j\}_{j\in G}$ ($G$ a discrete The maximum number of intersections between two plane rectangular paths We show that the maximum number of intersections between two plane rectangular paths with lengthsm andn, 2≤m≤n, is 4n+2, ifm=4 andn≡1(mod 3); and it ismn+1 otherwise. 更多
 In industry and in laboratory work oftentimes we are confronted with the problem of electromagnetic shielding between two bodies. In many ceases it is sufficient to have electrostatic shielding, and thus the interaction between two bodies can be determined by examining the mutual capacitance between them. When the interfering body is small and can be considered as a point source, its effect in the presence of another grounded conductor (in our case, the metallic shield) can be calculated by... In industry and in laboratory work oftentimes we are confronted with the problem of electromagnetic shielding between two bodies. In many ceases it is sufficient to have electrostatic shielding, and thus the interaction between two bodies can be determined by examining the mutual capacitance between them. When the interfering body is small and can be considered as a point source, its effect in the presence of another grounded conductor (in our case, the metallic shield) can be calculated by means of the Green's function for this grounded conductor surface. As the Green's functions for various surfaces are well established so these various forms of shielding can be handled by the method proposed in this paper. 在工业上和在实验室中,我们都会遇到两个物体之间的电磁屏蔽的问题。在许多应用中,我们只须注意到两个物体之间的静电屏蔽就够了,因而它们之间的相互作用可以从计算它们之间的相互电容来定出。当干扰物体的尺寸很小因而可以认为是一个点电源时,则当它与另一个接地导体(即问题中的电磁屏蔽)共同存在时所生的效应即可由这一个接地导体的格林函数表出。关于格林函数的知识已有很丰富的积累,因而本文中所提出的方法是可以解决多种多样的问题的。 文中讨论了扁椭球坐标和长椭球坐标中的格林函数,并对带虚数自变数的勒讓特函数的若干个公式作了推导,因为这些有用的公式在流行的文献中还未见到。 导体表面任意形状的小孔的问题是值得讨论的,特别是有限大导体表面上的小孔问题,本文从理论上验证了文献上已经提出来的实验结果。最后我们给出如下两个物体之间的相互电容公式:其中一个是在带小孔的闭合电磁屏蔽体的另一个之内。 In this article a dynamical theory of the heat transport process is developed. The concept of temperature difference between subsystems is introduced through the temperatures when they are disconnected and each of them is in equilibrium; we then treat the interaction between two subsystems as a perturbation. The rigorous expression of the coefficient of heat conductivity is obtained. For a large and uniform system, it is reduced to Kubo's formula. 本文由温度不同之平衡系统引入温度差的概念,以其边界接触作用为微扰,对热的输运过程进行了动力学的讨论。得到了热导系数的准确表示式。对于体积大的均匀系统,所得的公式简化为Kubo的公式。 A detailed study of the relation between diffraction points of various rhombohedral types and the type 6H of silicon carbide has been made, using the reciprocal lattice method. It was shown that there occur twelve possible relations. A method was proposed for determining the number of the close hexagonal packed layers in unit cell from the relations derived and the numbers of point between two Laue points of the type 6H. 本文根据倒易点阵原理,详细分析了碳化硅劳埃照相中各种SiC三方多型体斑点和SiC基本类型6H斑点间的相互配置关系。这种关系共总结出不外乎十二种,本文提出利用这种关系,以及两6H类型斑点(hOl)间未知三方多型体的斑点数目,来计算未知多型体类型层数的方法。 利用这一方法,对在实验室条件下以升华法制备的若干碳化硅单晶体进行了分析,发现了两种同时与6H类型连生的新的碳化硅高层多型体417R和453R,其空间群为R3m(C_(3v)~5,点阵参数以六方晶胞表示时为 417R:αH=3.0806A,c=1050.7A,z=417; 453R:αH=3.0806A,c=1141.4A,z=453。以三方晶胞描述时则为 417:αR=350.4A,α=30.4′z=139; 453R:αR=380.6A,α=27.8′,z=151。 << 更多相关文摘
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