Feynman diagrams and the large charge expansion in dimensions
arXiv:1911.08505 · doi:10.1016/j.physletb.2020.135202
Abstract
In arXiv:1909.01269 it was shown that the scaling dimension of the lightest charge operator in the model at the Wilson-Fisher fixed point in can be computed semiclassically for arbitrary values of , where is the perturbatively small fixed point coupling. Here we generalize this result to the fixed point of the model in dimensions. The result interpolates continuously between diagrammatic calculations and the universal conformal superfluid regime for CFTs at large charge. In particular it reproduces the expectedly universal contribution to the scaling dimension of large charge operators in CFTs.
arXiv comment7 pages, v2 typos fixed, match journal version
References in corpus (17)
- EPFL Lectures on Conformal Field Theory in D>= 3 Dimensions
- Semiclassics, Goldstone Bosons and CFT data
- Compensating strong coupling with large charge
- TASI Lectures on the Conformal Bootstrap
- The Epsilon Expansion Meets Semiclassics
- Low-Energy Quantum Effective Action for Relativistic Superfluids
- Summing tree graphs at threshold
- Conformal dimensions via large charge expansion
- Conformal Bootstrap At Large Charge
- On the CFT Operator Spectrum at Large Global Charge
- Semiclassical approach for multiparticle production in scalar theories
- Large charge at large N
- Higgsplosion: Solving the Hierarchy Problem via rapid decays of heavy states into multiple Higgs bosons
- Rotating superfluids and spinning charged operators in conformal field theory
- Observables in Inhomogeneous Ground States at Large Global Charge
- Inconsistencies of higgsplosion
- Non-Perturbative Aspects of Multiparticle Production
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