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A Study into the Possibility of Field Focusing Using 'Left-Handed' Materials

机译:使用“左手”材料进行场聚焦的可能性的研究

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The problem of focusing fluxes of electromagnetic field energy in the presence of structures of "left-handed" matter (LHM) assumed a special importance in the light of recent idea of Prof. J.B. Pendry [1] that a parallel-sided slab of LHM under certain conditions (ε = μ = -1) may serve as a "superlens" with unique focusing properties, whose resolution is not restricted by the well-known diffraction limit. The phenomenon is expected to exist owing to amplification of evanescent modes in an LHM-slab, which exponentially decay in ordinary media. Papers with argumented objections were published (in particular, [2, 3]); however, some researchers did not recognize these objections as being exhaustive and convincing and, for all we know, this scientific discussion is far from being finished. In order to solve the problem of the quality limit of focusing of the image of a point source utilizing the realistic finite-width dissipative LHM-slab, we used numerical methods to investigate the spatial distribution of components of electromagnetic field and its major characteristics (in particular, the Poynting vector) under conditions of excitation of a slab by one and two filamentary sources spaced some small distance apart. The solution was obtained by the method of volume integral equations using the Green's function of free space, with the slab parameters ε = μ ≈ -1 included in the expressions for polarization currents. This solution (as distinct, for example, from eigenfunction expansions or surface integral equations) does not at all involve the concept of the propagation coefficient of an LHM-filled space and is not associated with the use of other multiple valued functions whose arguments would include (possibly negative) permittivity and permeability. Moreover, the polarization currents singled out in the Maxwell equations may be identified with actually existing currents in the inclusions of the composite whose model is provided by LHM. Therefore, the method of volume integral equations offers a good tool for checking assumptions and testing solutions obtained by other methods.
机译:鉴于JB Pendry教授[1]的最新观点,即LHM的平行侧平板,在存在“左手”物质(LHM)结构的情况下聚焦电磁场能量通量的问题特别重要。在某些条件下(ε=μ= -1)可以用作具有独特聚焦特性的“超透镜”,其分辨率不受众所周知的衍射极限的限制。预计该现象将由于LHM平板中渐逝模式的放大而存在,而这种消失模式在普通介质中呈指数衰减。发表有异议的论文(特别是[2,3]);但是,一些研究人员并未意识到这些反对意见是详尽无遗的,并且令人信服,而且,就我们所知,这场科学讨论还远远没有结束。为了解决利用现实的有限宽度耗散LHM平板对点源图像聚焦的质量限制问题,我们使用数值方法研究了电磁场分量的空间分布及其主要特征(在特别地,在由一个和两个丝状源激发平板的条件下以一定的小距离隔开的Poynting向量。该解决方案是通过使用自由空间的格林函数的体积积分方程法获得的,其中平板参数ε=μ≈-1包含在极化电流的表达式中。该解决方案(例如,与本征函数展开式或表面积分方程式不同)完全不涉及LHM填充空间的传播系数的概念,并且与其他多值函数的使用无关,这些函数的参数将包括(可能为负)介电常数和磁导率。此外,可以用模型中由LHM提供的复合材料的夹杂物中的实际存在的电流来识别在麦克斯韦方程中选出的极化电流。因此,体积积分方程法为检查假设和检验其他方法获得的解提供了一个很好的工具。

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