't Hooft anomalies for staggered fermions
Simon Catterall

TL;DR
This paper explores how exact anomalies in staggered fermion theories influence their phase structure, revealing anomaly cancellation conditions that relate to topological phases and symmetric mass generation, with implications for lattice models and GUT theories.
Contribution
It demonstrates the role of 't Hooft anomalies in understanding staggered fermion phase structure and constructs a lattice model related to Pati-Salam GUT.
Findings
Existence of a perturbative anomaly breaking U(1) to Z4.
A 't Hooft anomaly that constrains fermion content for anomaly cancellation.
Connection between anomaly cancellation and topological superconductor boundary states.
Abstract
We show that the phase structure of certain staggered fermion theories can be understood on the basis of exact anomalies. These anomalies arise when staggered fermions are coupled to gravity which can be accomplished by replacing them by discrete K\"{a}hler-Dirac fermions. We first show the existence of a perturbative anomaly in even dimensions which breaks an exact symmetry of the massless theory down to . If we attempt to gauge this symmetry we find a 't Hooft anomaly which can only be cancelled for multiples of two K\"{a}hler-Dirac fields. This result is consistent with the cancellation of a further mixed non-perturbative 't Hooft anomaly between the global and a reflection symmetry. In four dimensional flat space, theories of two staggered fields yield eight Dirac or sixteen Majorana fermions in the continuum limit and this critical number of fermions agrees…
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Taxonomy
TopicsQuantum Chromodynamics and Particle Interactions · Atomic and Subatomic Physics Research · Particle physics theoretical and experimental studies
