Renormalization Group, Effective Action and Grand Unification Theories in Curved Space-Time

1991 ◽  
Vol 39 (8) ◽  
pp. 621-641 ◽  
Author(s):  
Sergei D. Odintsov
1990 ◽  
Vol 05 (20) ◽  
pp. 1599-1604 ◽  
Author(s):  
I.L. BUCHBINDER ◽  
I.L. SHAPIRO ◽  
E.G. YAGUNOV

GUT’s in curved space-time is considered. The set of asymptotically free and asymptotically conformally invariant models based on the SU (N) gauge group is constructed. The general solutions of renormalization group equations are considered as the special ones. Several SU (2N) models, which are finite in flat space-time (on the one-loop level) and asymptotically conformally invariant in external gravitational field are also presented.


2017 ◽  
pp. 217-244
Author(s):  
I. L. Buchbinder ◽  
S. D. Odintsov ◽  
I. L. Shapiro

1993 ◽  
Vol 08 (10) ◽  
pp. 1787-1796 ◽  
Author(s):  
I.L. SHAPIRO ◽  
E.G. YAGUNOV

New set of one-loop finite GUT models is constructed. In particular there are some SU (N), N=5, 7, 9…models with two Higgs multiplets. The stability of finite solutions in UV and IR limits is investigated. The asymptotical behavior of the effective Yukawa and scalar couplings verify the asymptotical finiteness of the models. The renormalization group equations in curved space-time are also considered.


1998 ◽  
Vol 117 (1) ◽  
pp. 1208-1213 ◽  
Author(s):  
V. Ch. Zhukovskii ◽  
I. V. Mamsurov

Author(s):  
Iosif L. Buchbinder ◽  
Ilya L. Shapiro

As the main purpose of renormalization is not to remove divergences but to get essential information about the finite part of effective action, this chapter discusses some of the existing methods of solving this problem; such methods can be denoted the renormalization group. First, the minimal subtraction renormalization group in curved space is formulated. Next, the chapter shows how the overall μ‎-independence of the effective action enables one to interpret μ‎-dependence in some situations. As an example, the effective potential is restored from the renormalization group and compared with the expression calculated directly in chapter 13. In addition, the global conformal (scaling) anomaly is derived from the renormalization group.


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