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The nonperturbative propagator and vertex in massless quenched QEDd

A Bashir1,2 and R Delbourgo2

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It is well known how multiplicative renormalizability of the fermion propagator, through its Schwinger–Dyson equation, imposes restrictions on the 3-point fermion–boson vertex in massless quenched quantum electrodynamics in four dimensions. Moreover, perturbation theory serves as an excellent guide for possible nonperturbative constructions of Green functions. We extend these ideas to arbitrary dimensions d. The constraint of multiplicative renormalizability of the fermion propagator is generalized to a Landau–Khalatnikov–Fradkin transformation law in d dimensions and it naturally leads to a constraint on the fermion–boson vertex. We verify that this constraint is satisfied in perturbation theory at the one-loop level in three dimensions. Based upon one-loop perturbative calculation of the vertex, we find additional restrictions on its possible nonperturbative forms in arbitrary dimensions.


PACS

12.20.Ds Specific calculations

11.15.Tk Other nonperturbative techniques

11.10.Gh Renormalization

MSC

81V10 Electromagnetic interaction; quantum electrodynamics

81T16 Nonperturbative methods of renormalization

81T17 Renormalization group methods

Subjects

Particle physics and field theory

Dates

Issue 25 (25 June 2004)

Received 20 February 2004

Published 9 June 2004



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