Abstract
In this paper we show, for the first time, that charged-hadron masses can be calculated on the lattice without relying on gauge fixing at any stage of the calculations. In our simulations we follow a recent proposal and formulate full QCD+QED on a finite volume, without spoiling locality, by imposing C-periodic boundary conditions in the spatial directions. Electrically charged states are interpolated with a class of operators, originally suggested by Dirac and built as functionals of the photon field, that are invariant under local gauge transformations. We show that the quality of the numerical signal of charged-hadron masses is the same as in the neutral sector and that charged-neutral mass splittings can be calculated with satisfactory accuracy in this setup. We also discuss how to describe states of charged hadrons with real photons in a fully gauge-invariant way by providing a first evidence that the proposed strategy can be numerically viable.
| Original language | English |
|---|---|
| Article number | 146 |
| Journal | Journal of High Energy Physics |
| Volume | 2018 |
| Issue number | 5 |
| Number of pages | 19 |
| ISSN | 1126-6708 |
| DOIs | |
| Publication status | Published - 1. May 2018 |
Funding
This work is part of the programme of the RC⋆ Collaboration and we warmly thank our colleagues for their help. We are particularly indebted to Alberto Ramos for his contribution to various stages of this work. BL is supported in part by the Royal Society, by the Wolf-son Foundation and by the STFC Consolidated Grants ST/L000369/1 and ST/P00055X/1. MH is supported by the Danish National Research Foundation grant DNRF90 and by a Lundbeck Foundation Fellowship grant. Numerical simulations have been performed on clusters of the Supercomputing Wales project, partly funded by the European Regional Development Fund (ERDF) via Welsh Government, on a cluster at CERN, managed by the HPC team in the IT Department, and on the Marconi system at CINECA under the initiative INFN-LQCD123.
Keywords
- Lattice Quantum Field Theory
- Nonperturbative Effects
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