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Main Author: Vitouladitis, Stathis
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2507.01104
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author Vitouladitis, Stathis
author_facet Vitouladitis, Stathis
contents We establish a state-operator correspondence for a class of non-conformal quantum field theories with continuous higher-form symmetries and a mixed anomaly. Such systems can always be realised as a relativistic superfluid. The symmetry structure induces an infinite tower of conserved charges, which we construct explicitly. These charges satisfy an abelian current algebra with a central extension, generalising the familiar Kac-Moody algebras to higher dimensions. States and operators are organised into representations of this algebra, enabling a direct correspondence. We demonstrate the correspondence explicitly in free examples by performing the Euclidean path integral on a $d$-dimensional ball, with local operators inserted in the origin, and matching to energy eigenstates on $S^{d-1}$ obtained by canonical quantisation. Interestingly, in the absence of conformal invariance, the empty path integral prepares a squeezed vacuum rather than the true ground state.
format Preprint
id arxiv_https___arxiv_org_abs_2507_01104
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Higher-form anomalies and state-operator correspondence beyond conformal invariance
Vitouladitis, Stathis
High Energy Physics - Theory
We establish a state-operator correspondence for a class of non-conformal quantum field theories with continuous higher-form symmetries and a mixed anomaly. Such systems can always be realised as a relativistic superfluid. The symmetry structure induces an infinite tower of conserved charges, which we construct explicitly. These charges satisfy an abelian current algebra with a central extension, generalising the familiar Kac-Moody algebras to higher dimensions. States and operators are organised into representations of this algebra, enabling a direct correspondence. We demonstrate the correspondence explicitly in free examples by performing the Euclidean path integral on a $d$-dimensional ball, with local operators inserted in the origin, and matching to energy eigenstates on $S^{d-1}$ obtained by canonical quantisation. Interestingly, in the absence of conformal invariance, the empty path integral prepares a squeezed vacuum rather than the true ground state.
title Higher-form anomalies and state-operator correspondence beyond conformal invariance
topic High Energy Physics - Theory
url https://arxiv.org/abs/2507.01104