Abstract
Second-order phase transitions are studied for a biaxial anisotropic disordered system composed of randomly distributed metal and non-metal regions, the former having tensor-type conductivity along the principal axes. Integrals are derived for the anisotropic Hall and Seebeck coefficients using Green functions. Computer calculations show that near the percolation threshold, the decrease of the biaxial anisotropy of the effective conductivity and Hall and Seebeck coefficients is described by new critical exponents. A model of 'special points' of the biaxial anisotropic infinite cluster above the threshold and the two-component infinite cluster below the threshold is developed.

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