Verification of mass shell Ward identities for gluons in the axial gauge

1978 ◽  
Vol 47 (4) ◽  
pp. 546-554 ◽  
Author(s):  
W. Konetschny
1982 ◽  
Vol 25 (4) ◽  
pp. 1002-1008 ◽  
Author(s):  
D. M. Capper ◽  
George Leibbrandt

1993 ◽  
Vol 71 (5-6) ◽  
pp. 252-255
Author(s):  
R. Kobes ◽  
G. Kunstatter ◽  
K. Mak

The calculation of the massless fermion damping rate to order g2T in the long-wavelength limit of hot gauge theories using the recently developed resummation methods in terms of hard thermal loops is reviewed. Ward identities between the effective propagators and vertices are used to formally prove the gauge independence of the damping rate to this order in a wide class of gauges. We also discuss some aspects of the cutoff dependence of the gauge-dependent terms proportional to the mass-shell condition.


2000 ◽  
Vol 15 (14) ◽  
pp. 2153-2179 ◽  
Author(s):  
M. SIMIONATO

We give a Wilsonian formulation of non-Abelian gauge theories explicitly consistent with axial gauge Ward identities. The issues of unitarity and dependence on the quantization direction are carefully investigated. A Wilsonian computation of the one-loop QCD beta function is performed.


1982 ◽  
Vol 25 (4) ◽  
pp. 1009-1018 ◽  
Author(s):  
D. M. Capper ◽  
George Leibbrandt

1986 ◽  
Vol 167 (4) ◽  
pp. 388-392 ◽  
Author(s):  
G. Veneziano

2001 ◽  
Vol 16 (10) ◽  
pp. 1679-1701 ◽  
Author(s):  
B. SATHIAPALAN

We continue the discussion of our previous paper on writing down gauge-invariant interacting equations for a bosonic string using the loop variable approach. In the earlier paper the equations were written down in one higher dimension where the fields are massless. In this paper we describe a procedure for dimensional reduction that gives interacting equations for fields with the same spectrum as in bosonic string theory. We also argue that the on-shell scattering amplitudes implied by these equations for the physical modes are the same as for the bosonic string. We check this explicitly for some of the simpler equations. The gauge transformation of space–time fields induced by gauge transformations of the loop variables are discussed in some detail. The unintegrated (i.e. before the Koba–Nielsen integration), regularized version of the equations, are gauge invariant off-shell (i.e. off the free mass shell).


1977 ◽  
Vol 15 (1) ◽  
pp. 121-128 ◽  
Author(s):  
A. A. Golestaneh
Keyword(s):  

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