On the accuracy of approximate descriptions of discrete superpositions of Bessel beams in the generalized Lorenz-Mie theory

L. Ambrosio, Carlos Henrique da Silva Santos, Ivan Eduardo Lage Rodrigues
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引用次数: 1

Abstract

This paper aims to investigate one of the most important schemes, viz. the localized approximation (LA), for describing arbitrary-shaped beams in the generalized Lorenz-Mie theory. Our focus is on a specific class of non-diffracting beams called discrete frozen waves, which are constructed from superpositions of Bessel beams and can be designed to provide virtually any longitudinal intensity pattern of interest. Recently, the LA was applied to frozen waves allowing, for the first time, for the analysis of light scattering problems from spherical scatterers and the subsequent determination of the physical/optical quantities in optical trapping. Since the LA cannot be rigorously applied to Bessel beams, it is of interest to determine whether those results and predictions previously established in the literature are reliable or not. To do so, we rely on exact descriptions of frozen waves and establish the limits to the validity of such an approximation scheme. It is revealed that, although serious doubts can be raised against its use, specially due to cumulative errors, the LA is much more robust than previously thought, and it may serve well to both paraxial and non-paraxial Frozen Waves, under certain circumstances.
广义洛伦兹-米理论中贝塞尔光束离散叠加态近似描述的准确性
本文的目的是研究广义洛伦兹-米氏理论中描述任意形状光束的最重要的格式之一,即局部化近似(LA)。我们的重点是一种特殊的非衍射光束,称为离散冻结波,它是由贝塞尔光束的叠加构成的,可以设计成几乎任何感兴趣的纵向强度模式。最近,LA首次应用于冻结波,用于分析球形散射体的光散射问题,并随后确定光捕获中的物理/光学量。由于LA不能严格地应用于贝塞尔光束,因此确定先前在文献中建立的这些结果和预测是否可靠是有意义的。为此,我们依赖于冻结波的精确描述,并确定这种近似方案有效性的限制。结果表明,尽管人们对其使用提出了严重的质疑,特别是由于累积误差,但LA比以前认为的要稳健得多,并且在某些情况下,它可以很好地适用于旁轴和非旁轴冻结波。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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