Universal scaling dimensions for highly irrelevant operators in the Local Potential Approximation

We study \(d\)-dimensional scalar field theory in the Local Potential Approximation of the functional renormalization group. Sturm-Liouville methods allow the eigenoperator equation to be cast as a Schrodinger-type equation. Combining solutions in the large field limit with the Wentzel-Kramers-Brill...

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Bibliographic Details
Published inarXiv.org
Main Authors Vlad-Mihai Mandric, Morris, Tim R, Stulga, Dalius
Format Paper Journal Article
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 14.11.2023
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ISSN2331-8422
DOI10.48550/arxiv.2306.14643

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Summary:We study \(d\)-dimensional scalar field theory in the Local Potential Approximation of the functional renormalization group. Sturm-Liouville methods allow the eigenoperator equation to be cast as a Schrodinger-type equation. Combining solutions in the large field limit with the Wentzel-Kramers-Brillouin approximation, we solve analytically for the scaling dimension \(d_n\) of high dimension potential-type operators \(\mathcal{O}_n(\varphi)\) around a non-trivial fixed point. We find that \(d_n = n(d-d_\varphi)\) to leading order in \(n\) as \(n \to \infty\), where \(d_\varphi=\frac{1}{2}(d-2+\eta)\) is the scaling dimension of the field, \(\varphi\), and determine the power-law growth of the subleading correction. For \(O(N)\) invariant scalar field theory, the scaling dimension is just double this, for all fixed \(N\geq0\) and additionally for \(N=-2,-4,\ldots \,.\) These results are universal, independent of the choice of cutoff function which we keep general throughout, subject only to some weak constraints.
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ISSN:2331-8422
DOI:10.48550/arxiv.2306.14643