Thermal free energy of large QED in dimensions from weak to strong coupling
In 2+1 dimensions, QED becomes exactly solvable for all values of the fermion charge e in the limit of many fermions >> 1. We present results for the free energy density at finite temperature T 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 O(e6N$$^{3}_{f}$$/ε), which we argue would become a finite contribution of order O(e6N$$^{4}_{f}$$) when resumming formally higher-order 1/ contributions. Still in the limit of large , we find the finite-temperature free energy to be well-behaved for all values of the dimensionless coupling e2Nf/T, and to be bounded from above by the free energy of free fermions and bounded from below by non-interacting QED3. We invite follow-up studies from finite-temperature lattice gauge theory at large but fixed to test our results in the regime e2 /T >> 1.
- Research Organization:
- Univ. of Colorado, Boulder, CO (United States)
- Sponsoring Organization:
- USDOE Office of Science (SC), Nuclear Physics (NP)
- Grant/Contract Number:
- SC0017905
- OSTI ID:
- 1571337
- Alternate ID(s):
- OSTI ID: 1593888
- Journal Information:
- Physical Review. D., Journal Name: Physical Review. D. Vol. 100 Journal Issue: 7; ISSN 2470-0010
- Publisher:
- American Physical Society (APS)Copyright Statement
- Country of Publication:
- United States
- Language:
- English
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