Abstract Using the Jones matrix formalism, crystal optical properties of inhomogeneous material consisting of a pile of weakly birefringent plates are analysed in relation to the cell model adopted in polarization tomography of 3D dielectric tensor field in photoelastic media. It is shown that the material manifests in general an “apparent” optical gyration caused by different orientations of the plates. Relations between the polarimetric parameters and the dielectric tensor components are ascertained for the case of weak optical anisotropy. Key words : photoelasticity, 3D tensor field tomography, birefringence, gyration, Jones matrices. PACS: 07.60.Fs, 42.25.Lc, 42.30.Wb Introduction Photoelasticity has been remaining one of extensively explored topics within the physical optics during the last decades (see, e.g., [1-4]). Its problems become enormously complicated if external (or internal) mechanical stresses are arbitrarily and inhomogeneously distributed inside a sample under test, thus transforming initially isotropic, macroscopically uniform material into anisotropic and homogeneous one. This field is often referred to as a 3D photoelasticity. In case of weakly anisotropic, weakly inhomogeneous materials possessing none or slight absorption, the stressed state manifests itself mainly in a notable effect on the polarization of probing light wave. Then the 3D spatial distribution of stresses (or, equivalently, that of dielectric parameters at the optical frequencies) might be clarified, using the methods of polarization optical tomography of 3D tensor fields (see [1,3]). In spite of essential current progress, those methods have not yet succeeded in solving the problem in its most general form. Considerable analytical difficulties of the tensor field tomography have stipulated a number of approximate approaches, e.g., a “discretely inhomogeneous” (or “cell”) model of the stressed material (see [2,5]), in which the sample is divided into many identical uniform cells. For a given propagation direction, the light beam probes a pile of anisotropic cells characterised by different parameters. This situation reminds a canonical problem of crystal optics, propagation of light through the so-called composite retardation plates [6,7]. Hence, elaboration of the latter would contribute to a better understanding of principles, techniques Ukr. J. Phys. Opt. 2005, V6, №3 87
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