On applicability of T-matrix-like methods Victor G. Farafonov^1, Vladimir B. Il'in^2, and Andrey A. Loskutov^1 ^1 St.Petersburg University of Aerocosmic Instrumentation ^2 Astronomical Institute, St.Petersburg University Abstract The T-matrix method and its modifications are very popular now in applications of the light scattering theory (e.g., [1-3]). The method is based on: i) the integral representation of the scattering problem; ii) expansion of the fields (or their potentials) in terms of the spherical wavefunctions, and iii) solution of infinite systems of algebraic equations for expansion coefficients. Analytical investigation of the systems in the case of perfectly conducting particles was recently made in [3]. It was shown that only for ``weakly non-convex scatterers'' the Fredholm alternative is valid for the systems and their solution can be obtained by reduction. However, the T-matrix method is not known to work when the scatterer shape is essentially non-spherical. For instance, for spheroids numerical instability can arise already for the aspect ratio a/b > 4 [4], although spheroids, being smooth convex bodies, belong to the weakly non-convex ones. In this paper we analytically investigate the algebraic systems for dielectric axisymmetric particles in frame of a recently suggested modification of the T-matrix method [2]. It is demonstrated that the Fredholm alternative is valid for the same condition as in [3], and namely: s_1 < s_2, where $s_1$ is the distance from the coordinate origin to the farthest peculiarity of the scattered field, s_2 that to the nearest peculiarity of the internal field. The condition (1) is weaker than that of validity of the Rayleigh hypothesis (convergence of the expansions everywhere up to the border of scatterer) r_{\rm min} > s_1, \ \ r_{\rm max} < s_2, where r_{\rm min} and r_{\rm max} are the distances from the coordinate origin to the nearest and farthest points of the scatterer surface, respectively Our computations indicate that for spheroids the expansions of the scattered field in contrast to the internal one do not converge already for a/b > 2, although the tests for the scattered field in a distant zone (the optical theorem, reciprocity relation, etc. [1]) are satisfied with a high accuracy. For Chebyshev particles, both scattered and internal fields have peculiarities and the regions of convergence for the fields are found to be more close. Similar results should occur for the classical T-matrix method as well. Moreover we believe that any T-matrix-like method involving the above mentioned features i)--iii) can be considered as theoretically correct when the Rayleigh hypothesis is satisfied. If the condition of weak non-convexity is not valid the method should not work at all. In the intermediate region one must take the results of calculations with a care, in particular as concern the internal fields and the scattered fields close to particle surface. Note that in numerical realizations a reduction of the systems must be done and a problem that is different from the initial one is actually solved. As a consequence we observe that the conditions (1) and (2) rather approximately define the region of convergence. References 1. Mishchenko M.I. et al. (2000) Light Scattering by Non-Spherical Particles, Acad. Press. 2. Farafonov V.G. et al. (1999) JQSRT, v.63, p.205--215. 3. Kyurkchan A.G. (2000) Radiotech. Elektron., v.45, p.1078--1083. 4. Voshchinnikov N.V. et al. (2000) JQSRT, v.65, p.877--893. 5. Voshchinnikov N.V., Farafonov V.G. (1993) Astrophys. Space Sci., v.204, p.19--87. 6. Farafonov V.G. (1983) Diff. Equat. (Sov.), v.19, p.1765--1777.