Consistent treatment of the infrared singularities in Coulomb-gauge two-dimensional quantum chromodynamics

1981 ◽  
Vol 23 (2) ◽  
pp. 397-416
Author(s):  
R. L. Stuller
1978 ◽  
Vol 133 (3) ◽  
pp. 435-460 ◽  
Author(s):  
Probir Roy ◽  
Gautam Bhattacharya

1994 ◽  
Vol 09 (07) ◽  
pp. 1067-1096 ◽  
Author(s):  
L. V. AVDEEV ◽  
D. I. KAZAKOV ◽  
I. N. KONDRASHUK

We investigate the possibility of generalizing the differential renormalization of D. Z. Freedman, K. Johnson and J. I. Latorre in an invariant fashion to theories with infrared divergencies via an infrared [Formula: see text] operation. Two-dimensional σ models and the four-dimensional ɸ4-theory diagrams with exceptional momenta are used as examples, while dimensional renormalization serves as a test scheme for comparison. We write the basic differential identities of the method simultaneously in co-ordinate and momentum space, introducing two scales which remove ultraviolet and infrared singularities. A consistent set of Fourier-transformation formulae is derived. However, the values for tadpole-type Feynman integrals in higher orders of perturbation theory prove to be ambiguous, depending on the order of evaluation of the subgraphs. In two dimensions, even earlier than this ambiguity manifests itself, renormalization-group calculations based on the infrared extension of differential renormalization lead to incorrect results. We conclude that the procedure of extended differential renormalization does not perform the infrared [Formula: see text] operation in a self-consistent way.


1985 ◽  
Vol 153 (1-2) ◽  
pp. 97-100 ◽  
Author(s):  
R.E. Gamboa Saraví ◽  
C.M. Naón ◽  
F.A. Schaposnik

1977 ◽  
Vol 15 (10) ◽  
pp. 2913-2914 ◽  
Author(s):  
Paul Federbush ◽  
Anthony Tromba

2015 ◽  
Vol 30 (17) ◽  
pp. 1550100 ◽  
Author(s):  
Davide R. Campagnari ◽  
Hugo Reinhardt

We study the static gluon and quark propagator of the Hamiltonian approach to quantum chromodynamics in Coulomb gauge in one-loop Rayleigh–Schrödinger perturbation theory. We show that the results agree with the equal-time limit of the four-dimensional propagators evaluated in the functional integral (Lagrangian) approach.


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