TY - JOUR
T1 - Renormalization-group-invariant 1/N corrections to nontrival φ4 theory
AU - Smekal, L.V.
AU - Langfeld, K.
AU - Reinhardt, H.
AU - Langbein, R.F.
PY - 1994
Y1 - 1994
N2 - In the framework of path integral linearization techniques, the effective potential and the master field equation for massless 4 theory, in the modified loop expansion around the mean field, are derived up to next to leading order. In the O(N)-symmetric theory, these equations are equivalent to a subsummation of O(N) and order 1 diagrams. A renormalization prescription is proposed which is manifestly renormalization group invariant. The numerical results for the potential in next to leading order agree qualitatively well with the leading order ones. In particular, the nontrivial phase structure remains unchanged. Quantitatively, the corrections ar small for N 8, but even for N as small as one their essential effect is to modify the scaling coefficient 0 in the Callan-Symanzik function, in accordance with conventional loop expansions. The numerical results are best parametrized by scaling improved mean field formulas. Dimensional transmutation renders the overall (physical) mass scale M0, generated by a dynamical breaking of scale invariance, the only adjustable parameter of the theory. Renormalization group invariance of the numerical results is explicitly verified.
AB - In the framework of path integral linearization techniques, the effective potential and the master field equation for massless 4 theory, in the modified loop expansion around the mean field, are derived up to next to leading order. In the O(N)-symmetric theory, these equations are equivalent to a subsummation of O(N) and order 1 diagrams. A renormalization prescription is proposed which is manifestly renormalization group invariant. The numerical results for the potential in next to leading order agree qualitatively well with the leading order ones. In particular, the nontrivial phase structure remains unchanged. Quantitatively, the corrections ar small for N 8, but even for N as small as one their essential effect is to modify the scaling coefficient 0 in the Callan-Symanzik function, in accordance with conventional loop expansions. The numerical results are best parametrized by scaling improved mean field formulas. Dimensional transmutation renders the overall (physical) mass scale M0, generated by a dynamical breaking of scale invariance, the only adjustable parameter of the theory. Renormalization group invariance of the numerical results is explicitly verified.
UR - http://www.scopus.com/inward/record.url?eid=2-s2.0-0007272141&partnerID=MN8TOARS
UR - https://go.openathens.net/redirector/westernsydney.edu.au?url=https://doi.org/10.1103/PhysRevD.50.6599
U2 - 10.1103/PhysRevD.50.6599
DO - 10.1103/PhysRevD.50.6599
M3 - Article
SN - 0556-2821
VL - 50
SP - 6599
EP - 6609
JO - Physical Review D
JF - Physical Review D
IS - 10
ER -