2 citations · 4 across the 7 of their papers we have counts for
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The Light Front Gauge Propagator: The Status Quo
A. T. Suzuki, J. H. O. Sales
At the classical level, the inverse differential operator for the quadratic term in the gauge field Lagrangian density fixed in the light front through the multiplier (nA)^2 yields…
Can two or more gauge bosons propagate in the light-front?
A. T. Suzuki, J. H. O. Sales
Gauge fields in the light-front are usually fixed via the nA=0 condition yielding the non-local singularities of the type (kn)^(-a)=0 and a=1,2,.. in the gauge boson propagator whi…
Light-front gauge propagator reexamined-II
Alfredo T. Suzuki, J. H. O. Sales
Gauge fields are special in the sense that they are invariant under gauge transformations and \emph{``ipso facto''} they lead to problems when we try quantizing them straightforwar…
Covariantization and canonical quantization in the light-cone gauge
Alfredo T. Suzuki, Ricardo Bentin
In the light-cone gauge choice for Abelian and non-Abelian gauge fields, the vector boson propagator carries in it an additional ``spurious'' or ``unphysical'' pole intrinsic to th…
Solutions for a massless off-shell two-loop three-point vertex
Alfredo T. Suzuki, Alexandre G. M. Schmidt
Negative dimensional integration method (NDIM) seems to be a very promising technique for evaluating massless and/or massive Feynman diagrams. It is unique in the sense that the me…
Negative Dimensional Integration for Massive Four Point Functions--II: New Solutions
Alfredo T. Suzuki, Alexandre G. M. Schmidt
In this sequel calculation of the one-loop Feynman integral pertaining to a massive box diagram contributing to the photon-photon scattering amplitude in quantum electrodynamics, w…