Finsleroid-relativistic time-asymmetric space and quantized fields

For well-defined Finsleroid-relativistic space epsilon(SR)(g) (with the superscript SR meaning special- relativistic) due only to accounting for a characteristic parameter g which measures the deviation of the geometry from its pseudoeuclidean precursor, the creation of the respective quantization programs for relativistic physical fields seems to be an urgent task. In the present work, the formulation of theory for relativistic physical fields in such a space is initiated. A general method to solve respective scalar, electromagnetic, and spinor field equations is proposed basing on the conformal flatness. At any value of the parameter, the expansion of the relativistic fields with respect to non-plane waves appeared is found, which proposes a base upon which the fields can be quantized in the context of the Finsleroid-relativistic approach. Remarkably, the regulators can naturally be proposed to overcome divergences in relativistic field integrals. The respective key and basic concepts involved are presented.