Effective Action for QED with Fermion Self-Interaction in D=2 and D=3 Dimensions
arXiv:hep-th/0201125 · doi:10.1103/PhysRevD.65.125030
Abstract
In this work we discuss the effect of the quartic fermion self-interaction of Thirring type in QED in D=2 and D=3 dimensions. This is done through the computation of the effective action up to quadratic terms in the photon field. We analyze the corresponding nonlocal photon propagators nonperturbatively in % \frac{k}{m}, where k is the photon momentum and m the fermion mass. The poles of the propagators were determined numerically by using the Mathematica software. In D=2 there is always a massless pole whereas for strong enough Thirring coupling a massive pole may appear . For D=3 there are three regions in parameters space. We may have one or two massive poles or even no pole at all. The inter-quark static potential is computed analytically in D=2. We notice that the Thirring interaction contributes with a screening term to the confining linear potential of massive QED_{2}. In D=3 the static potential must be calculated numerically. The screening nature of the massive QED prevails at any distance, indicating that this is a universal feature of % D=3 electromagnetic interaction. Our results become exact for an infinite number of fermion flavors.
Latex, 13 pages, 3 figures
References in corpus (1)
Cited by in corpus (6)
- Bosonization and Functional Renormalization Group Approach in the Framework of QED_2
- The static potential in QED with non-minimal coupling
- Static potential in scalar QED with non-minimal coupling
- Perturbative bosonization from two-point correlation functions
- A dual gravity study of the 2+1D compact U(1) gauge theory coupled with strongly interacting matter fields
- Fractional statistics and confinement