Renormalization Group, Asymptotic Freedom, And More... by Vsemayr A. Shakhbazyan

See the text.

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.