Email Vsemayr A. Shakhbazyan at twc7184609354@earthlink.net

*You
must remove the functional
arbitrariness from the RG-equations
when you return to the physical theory.
*

*
Because of that process, the RG-equations transform to
identities, and the "ghost states"
completely disappear from the conventional
models of the Quantum Field Theory.
*

*
This transition is equivalent to imposing
a "natural boundary condition"
to the asymptotical behavior of the
effective interaction. *

*
As always in mathematical physics, then something new
appears: *

*the
non-perturbative asymptotically free
solution pops
up. *

*
See the text. *