Flows in the space of interacting chiral boson theories

We study interacting theories of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>N</a:mi></a:math> left-moving and <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mover accent="true"><c:mi>N</c:mi><c:mo stretchy="false">¯</c:mo></c:mover></c:math> right-moving Floreanini-Jackiw bosons in two dimensions. A parametrized family of such theories is shown to enjoy (nonmanifest) Lorentz invariance if and only if its Lagrangian obeys a flow equation driven by a function of the energy-momentum tensor. We discuss the canonical quantization of such theories along classical stress tensor flows, focusing on the case of the root-<g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>T</g:mi><g:mover accent="true"><g:mi>T</g:mi><g:mo stretchy="false">¯</g:mo></g:mover></g:math> deformation, where we obtain perturbative results for the deformed spectrum in a certain large-momentum limit. In the special case <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mi>N</k:mi><k:mo>=</k:mo><k:mover accent="true"><k:mi>N</k:mi><k:mo stretchy="false">¯</k:mo></k:mover></k:math>, we consider the quantum effective action for the root-<o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>T</o:mi><o:mover accent="true"><o:mi>T</o:mi><o:mo stretchy="false">¯</o:mo></o:mover></o:math>-deformed theory by expanding around a general classical background, and we find that the one-loop contribution vanishes for backgrounds with constant scalar gradients. Our analysis can also be interpreted via dual <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"><s:mi>U</s:mi><s:mo stretchy="false">(</s:mo><s:mn>1</s:mn><s:mo stretchy="false">)</s:mo></s:math> Chern-Simons theories in three dimensions, which might be used to describe deformations of charged <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"><w:msub><w:mi>AdS</w:mi><w:mn>3</w:mn></w:msub></w:math> black holes or quantum Hall systems. Published by the American Physical Society 2024

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2024-08-05
DOI
https://doi.org/10.1103/physrevd.110.046005
Citations
11
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
7.26

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article

Flows in the space of interacting chiral boson theories

Christian Ferko, Gabriele Tartaglino‐Mazzucchelli, Stephen Ebert, Cian Luke Martin
11 citations
Physical review. D/Physical review. D.
Black Holes and Theoretical Physics
7.26
article

Flows in the space of interacting chiral boson theories

Christian Ferko, Gabriele Tartaglino‐Mazzucchelli, Stephen Ebert, Cian Luke Martin
article en
11 citations

Abstract

We study interacting theories of <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>N</a:mi></a:math> left-moving and <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mover accent="true"><c:mi>N</c:mi><c:mo stretchy="false">¯</c:mo></c:mover></c:math> right-moving Floreanini-Jackiw bosons in two dimensions. A parametrized family of such theories is shown to enjoy (nonmanifest) Lorentz invariance if and only if its Lagrangian obeys a flow equation driven by a function of the energy-momentum tensor. We discuss the canonical quantization of such theories along classical stress tensor flows, focusing on the case of the root-<g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>T</g:mi><g:mover accent="true"><g:mi>T</g:mi><g:mo stretchy="false">¯</g:mo></g:mover></g:math> deformation, where we obtain perturbative results for the deformed spectrum in a certain large-momentum limit. In the special case <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mi>N</k:mi><k:mo>=</k:mo><k:mover accent="true"><k:mi>N</k:mi><k:mo stretchy="false">¯</k:mo></k:mover></k:math>, we consider the quantum effective action for the root-<o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>T</o:mi><o:mover accent="true"><o:mi>T</o:mi><o:mo stretchy="false">¯</o:mo></o:mover></o:math>-deformed theory by expanding around a general classical background, and we find that the one-loop contribution vanishes for backgrounds with constant scalar gradients. Our analysis can also be interpreted via dual <s:math xmlns:s="http://www.w3.org/1998/Math/MathML" display="inline"><s:mi>U</s:mi><s:mo stretchy="false">(</s:mo><s:mn>1</s:mn><s:mo stretchy="false">)</s:mo></s:math> Chern-Simons theories in three dimensions, which might be used to describe deformations of charged <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"><w:msub><w:mi>AdS</w:mi><w:mn>3</w:mn></w:msub></w:math> black holes or quantum Hall systems. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(4)
University of California, Los Angeles (US), The University of Queensland (AU), University of California System (US), University of California, Davis (US)
U.S. Department of Energy, University of California, University of Queensland, Australian Research Council, Kavli Institute for Theoretical Physics, University of California, Santa Barbara
Openalex Percentile: Top 2%
Black Holes and Theoretical Physics
7.26
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