Geometry of the Divergences Problem in QFT

The divergences problem in QFT should be overcame presumably due to the unification of the fundamental interactions [1]. We evidently cannot to achieve this goal now. Together with this there are divergences in problems where the highenergy processes simply cannot be involved (say electron self-energy, Lamb’s shift, etc.). Last ones reflect the formal character of perturbation theory applied to interacting secondly quantized amplitudes of the pointwise particles. These difficulties are borrowed partly from the classical theory. I would like to establish some general framework for the future unified theory avoiding to use the method of classical analogy. PASC: 03.65.Ca, 03.65.Ta, 04.20.Cv