scholarly journals HOW TO TREAT γ5

1998 ◽  
Vol 13 (17) ◽  
pp. 2991-3050 ◽  
Author(s):  
HUNG CHENG ◽  
S. P. LI

In the past two decades, Dyson's formalism of renormalization has been mostly superceded by dimensional regularization, particularly in the treatment of quantum gauge field theories with spontaneous symmetry breaking or those with chiral fermions. In this paper, we shall carry out explicitly Dyson's subtraction program, making it applicable to such field theories. In particular, we show with the example of the Abelian–Higgs theory how to handle amplitudes of chiral fermions. We show that these amplitudes which involve the γ5 matrix can be calculated in an unambiguous and gauge invariant way. This is done by establishing the subtraction conditions for the propagator of a chiral fermion as well as those for the VVV amplitude, when V denotes the vector meson. The renormalized constants are chosen to satisfy the Ward–Takahashi identities. As a demonstration, we calculate the next-lowest order correction of the anomaly in the Abelian–Higgs model and find that it vanishes.

1989 ◽  
Vol 323 (3) ◽  
pp. 493-512 ◽  
Author(s):  
William A. Bardeen ◽  
C.N. Leung ◽  
S.T. Love

2004 ◽  
Vol 19 (32) ◽  
pp. 5615-5624 ◽  
Author(s):  
J. M. GRIMSTRUP ◽  
B. KLOIBÖCK ◽  
L. POPP ◽  
M. SCHWEDA ◽  
M. WICKENHAUSER ◽  
...  

We discuss the different possibilities of constructing the various energy–momentum tensors for noncommutative gauge field models. We use Jackiw's method in order to get symmetric and gauge invariant stress tensors — at least for commutative gauge field theories. The noncommutative counterparts are analyzed with the same methods. The issues for the noncommutative cases are worked out.


1987 ◽  
Vol 02 (09) ◽  
pp. 663-674 ◽  
Author(s):  
D. I. KAZAKOV

In the present paper we give a detailed description of the method to construct finite N = 1 SUSY gauge field theories in the framework of N = 1 superfields within dimensional regularization. The finiteness of all the Green functions is based on supersymmetry and gauge invariance and is achieved by a proper choice of matter content of the theory and Yukawa couplings in the form yi = fi(ε)g, where g is the gauge coupling, and the function fi(ε) is regular at ε = 0 and is calculated in perturbation theory. Necessary and sufficient conditions for finiteness are determined already in the one-loop approximation. The correspondence with an earlier proposed approach to construct finite theories based on eigenvalue solutions of renormalization-group equations is established.


Sign in / Sign up

Export Citation Format

Share Document