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G. Gouesbet 《Optics Communications》2007,278(1):215-220
The (electromagnetic) generalized Lorenz-Mie theory describes the interaction between an electromagnetic arbitrary shaped beam and a homogeneous sphere. It is a generalization of the Lorenz-Mie theory which deals with the simpler case of a plane wave illumination. In a recent paper, we consider (i) elastic cross-sections in electromagnetic generalized Lorenz-Mie theory and (ii) elastic cross-sections in an associated quantum generalized Lorenz-Mie theory. We demonstrated that the electromagnetic problem is equivalent to a superposition of two effective quantum problems. We now intend to generalize this result from elastic cross-sections to inelastic cross-sections. A prerequisite is to build an asymptotic quantum inelastic generalized Lorenz-Mie theory, which is presented in this paper. 相似文献
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The generalized Lorenz-Mie theory in the strict sense describes the interaction between an illuminating arbitrary shaped beam and a homogeneous sphere characterized by its diameter d and its complex refractive index m. It relies on the method of separation of variables expressed in spherical coordinates. Other generalized Lorenz-Mie theories (for other kinds of scatterers) expressed in spherical coordinates are available too. In these theories, the illuminating beam is expressed by using expansions with expansion coefficients depending on some fundamental coefficients named beam shape coefficients, more specifically spherical beam shape coefficients. In this paper we present a general formulation for the transformation of spherical beam shape coefficients through rotations of coordinate systems. 相似文献
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Grard Gouesbet 《Particle & Particle Systems Characterization》1994,11(1):22-34
Many optical sizing techniques rely on particle/laser interactions. The classical Lorenz-Mie theory describing sphere/plane wave interactions is therefore misleading when designing instruments and processing data when the particle size is not small enough with respect to beam diameters. In such cases the use of the generalized Lorenz-Mie theory is required. After summarizing essential features of the generalized Lorenz-Mie theory for sphere/arbitray wave interactions, this paper describes applications of the theory with some emphasis on the analysis of phase-Doppler anemometers. 相似文献
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Grard Gouesbet 《Particle & Particle Systems Characterization》2003,20(6):382-386
The formulation of the Debye series ready for implementation in generalized Lorenz‐Mie theory (theory of interaction between an arbitrary shaped beam and a homogeneous sphere) is presented in the framework of the Bromwich method. 相似文献
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Grard Gouesbet 《Particle & Particle Systems Characterization》1997,14(2):88-92
In Part 1, it was demonstrated that intensity measurements on an actual beam in the laboratory allow one to determine so-called density matrices related to the beam shape coefficients encoding the beam and used in many expressions of the generalized Lorenz-Mie theory. In this paper, expressions in the generalized Lorenz-Mie theory are rewritten and it is shown that they can be expressed in terms of the density matrices rather than in terms of beam shape coefficients, leading to what is called the density matrix approach to the generalized Lorenz-Mie theory. The possibility of rewriting the generalized Lorenz-Mie theory in terms of quantities describing the illuminating beam and experimentally measurable in the laboratory offers new opportunities in optical characterization. 相似文献
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The theory of interaction between a shaped beam and an infinite cylinder arbitrarily located in it is presented. The same approach as for the generalized Lorenz-Mie theory is first used. In particular, variable separability is assumed in solving the wave equation. The special case of Gaussian beams, however, implies that, unexpectedly, a special class of non-separable scalar potentials is required for some kinds of beams. 相似文献
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G. Gouesbet 《Optics Communications》2010,283(4):517-4466
There has been recently a growing interest in the development of what is usually known as the T-matrix method (better to be named: T-matrix formulation), in connection with studies concerning light scattering by nonspherical particles. Another line of research has been devoted to the development of generalized Lorenz-Mie theories dealing with the interaction between arbitrary electromagnetic shaped beams and some regular particles, allowing one to solve Maxwell’s equations by using a method of separation of variables. Both lines of research are conjointly considered in this paper. Results of generalized Lorenz-Mie theories in spherical coordinates (for homogeneous spheres, multilayered spheres, spheres with an eccentrically located spherical inclusion, assemblies of spheres and aggregates) are modified from scalar results in the framework of the Bromwich method to vectorial expressions using vector spherical wave functions (VSWFs) in order to match the T-matrix formulation, and to express the T-matrix. The results obtained are used as a basis to clarify statements, some of them erroneous, concerning the T-matrix formulation and to provide recommendations for better terminologies. 相似文献
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The generalized Lorenz–Mie theories for a homogeneous sphere (interaction between an electromagnetic arbitrary shaped beam and a sphere defined by its diameter and its complex refractive index), and for other particles as well (such as cylindrical particles, with circular or elliptical cross-sections) have been developed by using the Bromwich method. Conversely, this method cannot be used for spheroidal particles. Whether it is possible or not to use the Bromwich method implies a certain number of consequences concerning (i) the definition of TM- and TE-waves, (ii) the definition of genuine beam shape coefficients to describe the beam, (iii) the possibility of developing a localized beam model to describe the illuminating beam. These three issues may be enlightened by referring to the properties of the Bromwich method. 相似文献
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Huayong Zhang 《Journal of Quantitative Spectroscopy & Radiative Transfer》2011,112(9):1486-1491
A generalized Lorenz-Mie theory framework (GLMT) is applied to the study of Gaussian beam scattering by a spherical particle with an embedded spheroid at the center. By virtue of a transformation between the spherical and spheroidal vector wave functions, a theoretical procedure is developed to deal with the boundary conditions. Numerical results of the normalized differential scattering cross section are presented. 相似文献
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Based on the generalized Lorenz–Mie theory (GLMT), which provides the general framework and expansion of the incident shaped
beam in terms of cylindrical vector wave functions, an analytic solution to the electromagnetic scattering by coated infinite
cylinders is constructed for arbitrary incidence of a shaped beam. As an example, for a tightly focused Gaussian beam propagating
perpendicularly to the cylinder axis, the scattering characteristics that obviously demonstrate the three-dimensional nature
are described in detail, and numerical results of the normalized differential scattering cross section are evaluated. 相似文献