Interactions of massless fermionic fields in three dimensions

Fuente: arXiv
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Auteurs principaux: Fredenhagen, Stefan, Lausch, Filipp, Mkrtchyan, Karapet
Format: Preprint
Publié: 2024
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author Fredenhagen, Stefan
Lausch, Filipp
Mkrtchyan, Karapet
author_facet Fredenhagen, Stefan
Lausch, Filipp
Mkrtchyan, Karapet
contents All independent interaction vertices involving massless (Fang--Fronsdal) fermions in three dimensions are classified, completing the classification of interactions of massless fields of any spin. Similarly to the bosonic case, we get no independent vertices at quartic or higher order in the fields involving fields with spin $s\geq 3/2$, and cubic vertices only for spins satisfying triangle inequalities, apart from the cases involving (matter) fields with spin $s\leq 1$. Differently from the bosonic cases, we get only one vertex for each triple of spins with two Majorana fermions and one boson, which is parity even (odd) when the sum of the spins of all fields involved is odd (even). When the two Majorana fermions are identical, their coupling to an odd-spin boson is trivialized. We comment on the non-trivial holographic dictionary relating these vertices to $CFT$ correlators in two dimensions.
format Preprint
id arxiv_https___arxiv_org_abs_2404_00497
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Interactions of massless fermionic fields in three dimensions
Fredenhagen, Stefan
Lausch, Filipp
Mkrtchyan, Karapet
High Energy Physics - Theory
All independent interaction vertices involving massless (Fang--Fronsdal) fermions in three dimensions are classified, completing the classification of interactions of massless fields of any spin. Similarly to the bosonic case, we get no independent vertices at quartic or higher order in the fields involving fields with spin $s\geq 3/2$, and cubic vertices only for spins satisfying triangle inequalities, apart from the cases involving (matter) fields with spin $s\leq 1$. Differently from the bosonic cases, we get only one vertex for each triple of spins with two Majorana fermions and one boson, which is parity even (odd) when the sum of the spins of all fields involved is odd (even). When the two Majorana fermions are identical, their coupling to an odd-spin boson is trivialized. We comment on the non-trivial holographic dictionary relating these vertices to $CFT$ correlators in two dimensions.
title Interactions of massless fermionic fields in three dimensions
topic High Energy Physics - Theory
url https://arxiv.org/abs/2404.00497