Casimir energy on the sphere and 6D CFT trace anomaly

Fuente: arXiv
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Autori principali: Aros, R., Bugini, F., Díaz, D. E., Núñez-Barra, C.
Natura: Preprint
Pubblicazione: 2024
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author Aros, R.
Bugini, F.
Díaz, D. E.
Núñez-Barra, C.
author_facet Aros, R.
Bugini, F.
Díaz, D. E.
Núñez-Barra, C.
contents We elucidate the dependence of the Casimir energy on the trace anomaly coefficients for a six-dimensional CFT on $R\times S^5$. This extends the universal dependence on the central charge in 2D and the relation by Cappelli and Coste in 4D, unveiling the role of the trivial total derivatives in the anomaly that renders the Casimir energy scheme dependent. We obtain $$E_o=-\frac{15}{8}\,a_6 -\frac{5}{12}\,\left(g_5+\frac{1}{4}\,g_7+\frac{1}{2}\,g_8-10\, g_9+g_{10}\right),$$ with $a_6$ being the type A central charge and the $g$'s, the coefficients of five out of six terms that form a basis for trivial total derivatives. The derivation is based on the Polyakov formulas (conformal primitive) resulting from the integration of the trace anomaly. Alternatively, on a 6D conformally flat background the above basis is redundant and one can simplify further to get, in terms of the Schouten scalar $J$ and the Schouten tensor $V$, Branson's basis for trivial total derivatives $\nabla^2\nabla^2 J$, $\nabla^2J^2$ and $\nabla^2|V|^2+2\nabla\cdot(V\cdot\nabla\,J)$ with coefficients $γ_1, γ_2$ and $γ_3$, respectively, \begin{equation} \nonumber E_o=-\frac{15}{8}a_6-\frac{1}{24}\left(γ_1-γ_2 -\frac{1}{8}γ_3\right)~. \end{equation}
format Preprint
id arxiv_https___arxiv_org_abs_2404_15561
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Casimir energy on the sphere and 6D CFT trace anomaly
Aros, R.
Bugini, F.
Díaz, D. E.
Núñez-Barra, C.
High Energy Physics - Theory
General Relativity and Quantum Cosmology
Mathematical Physics
We elucidate the dependence of the Casimir energy on the trace anomaly coefficients for a six-dimensional CFT on $R\times S^5$. This extends the universal dependence on the central charge in 2D and the relation by Cappelli and Coste in 4D, unveiling the role of the trivial total derivatives in the anomaly that renders the Casimir energy scheme dependent. We obtain $$E_o=-\frac{15}{8}\,a_6 -\frac{5}{12}\,\left(g_5+\frac{1}{4}\,g_7+\frac{1}{2}\,g_8-10\, g_9+g_{10}\right),$$ with $a_6$ being the type A central charge and the $g$'s, the coefficients of five out of six terms that form a basis for trivial total derivatives. The derivation is based on the Polyakov formulas (conformal primitive) resulting from the integration of the trace anomaly. Alternatively, on a 6D conformally flat background the above basis is redundant and one can simplify further to get, in terms of the Schouten scalar $J$ and the Schouten tensor $V$, Branson's basis for trivial total derivatives $\nabla^2\nabla^2 J$, $\nabla^2J^2$ and $\nabla^2|V|^2+2\nabla\cdot(V\cdot\nabla\,J)$ with coefficients $γ_1, γ_2$ and $γ_3$, respectively, \begin{equation} \nonumber E_o=-\frac{15}{8}a_6-\frac{1}{24}\left(γ_1-γ_2 -\frac{1}{8}γ_3\right)~. \end{equation}
title Casimir energy on the sphere and 6D CFT trace anomaly
topic High Energy Physics - Theory
General Relativity and Quantum Cosmology
Mathematical Physics
url https://arxiv.org/abs/2404.15561