Non-Compact Pure Gauge QED in 3D is Free
arXiv:hep-th/9503225 · doi:10.1016/0370-2693(95)00913-6
Abstract
For all Poincaré invariant Lagrangians of the form , in three Euclidean dimensions, where is any invariant function of a non-compact field strength , we find that the only continuum limit (described by just such a gauge field) is that of free field theory: First we approximate a gauge invariant version of Wilson's renormalization group by neglecting all higher derivative terms in , but allowing for a general non-vanishing anomalous dimension. Then we prove analytically that the resulting flow equation has only one acceptable fixed point: the Gaussian fixed point. The possible relevance to high- superconductivity is briefly discussed.
11 pages, plain tex, uses harvmac. Minor additions - version to be published in Physics Letters B
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- Derivative expansion of the renormalization group in O(N) scalar field theory
- Gauge Invariance, the Quantum Action Principle, and the Renormalization Group
- Three dimensional massive scalar field theory and the derivative expansion of the renormalization group
- Large N and the renormalization group
- A Generalised Manifestly Gauge Invariant Exact Renormalisation Group for SU(N) Yang-Mills
- Asymptotic solutions in asymptotic safety
- A Manifestly Gauge Invariant, Continuum Calculation of the SU(N) Yang-Mills two-loop beta function
- Manifestly diffeomorphism invariant classical Exact Renormalization Group
- Properties of derivative expansion approximations to the renormalization group
- Triviality from the Exact Renormalization Group
- BRST in the Exact RG
- C Function Representation of the Local Potential Approximation
- Exact renormalization group study of fermionic theories
- Background independent exact renormalisation
- Provable properties of asymptotic safety in approximation
- General Computations Without Fixing the Gauge
- Functional flows in QED and the modified Ward-Takahashi identity
- Conformal anomaly from gauge fields without gauge fixing
- Two Phases for Compact U(1) Pure Gauge Theory in Three Dimensions
- Exact renormalization group approach in scalar and fermionic theories