Thermal free energy of large Nf QED in 2+1 dimensions from weak to strong coupling
arXiv:1908.09835 · doi:10.1103/PhysRevD.100.073009
Abstract
In 2+1 dimensions, QED becomes exactly solvable for all values of the fermion charge in the limit of many fermions . We present results for the free energy density at finite temperature to next-to-leading-order in large . In the naive large limit, we uncover an apparently UV-divergent contribution to the vacuum energy at order , which we argue to become a finite contribution of order when resumming formally higher-order contributions. We find the finite-temperature free energy to be well-behaved for all values of the dimensionless coupling , and to be bounded by the free energy of free fermions and non-interacting QED3, respectively. We invite follow-up studies from finite-temperature lattice gauge theory at large but fixed to test our results in the regime .
17 pages, 1 figure; comments welcome
References in corpus (8)
- Quantum criticality of U(1) gauge theories with fermionic and bosonic matter in two spatial dimensions
- More Abelian Dualities in 2+1 Dimensions
- Non-perturbative beta function in three-dimensional electrodynamics
- Simple non-perturbative resummation schemes beyond mean-field: case study for scalar theory in 1+1 dimensions
- Analytic Transport from Weak to Strong Coupling in the O(N) model
- Finite temperature CFT results for all couplings: O(N) model in 2+1 dimensions
- Fractionalized Degrees of Freedom at Infinite Coupling in large Nf QED in 2+1 dimensions
- Effective Coupling Constant of Plasmons
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