4.4 Article

Renormalized holographic entanglement entropy in Lovelock gravity

期刊

JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 6, 页码 -

出版社

SPRINGER
DOI: 10.1007/JHEP06(2021)073

关键词

AdS-CFT Correspondence; Classical Theories of Gravity; Gauge-gravity correspondence

资金

  1. FONDECYT [3190314, 1170765]
  2. ANID, REC Convocatoria Nacional Subvencion a Instalacion en la Academia Convocatoria Ano 2020 [PAI77200097]
  3. Natural Sciences and Engineering Research Council of Canada

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In this study, the renormalization of Entanglement Entropy in holographic CFTs dual to Lovelock gravity is investigated. A new renormalization prescription for the Jacobson-Myers functional is proposed through the Kounterterm renormalization procedure, which effectively cancels divergences in the EE for spherical entangling surfaces. This method provides C-function candidates for odd and even dimensional CFTs dual to Lovelock gravity without requiring limiting Einstein behavior of the theory.
We study the renormalization of Entanglement Entropy in holographic CFTs dual to Lovelock gravity. It is known that the holographic EE in Lovelock gravity is given by the Jacobson-Myers (JM) functional. As usual, due to the divergent Weyl factor in the Fefferman-Graham expansion of the boundary metric for Asymptotically AdS spaces, this entropy functional is infinite. By considering the Kounterterm renormalization procedure, which utilizes extrinsic boundary counterterms in order to renormalize the on-shell Lovelock gravity action for AAdS spacetimes, we propose a new renormalization prescription for the Jacobson-Myers functional. We then explicitly show the cancellation of divergences in the EE up to next-to-leading order in the holographic radial coordinate, for the case of spherical entangling surfaces. Using this new renormalization prescription, we directly find the C-function candidates for odd and even dimensional CFTs dual to Lovelock gravity. Our results illustrate the notable improvement that the Kounterterm method affords over other approaches, as it is non-perturbative and does not require that the Lovelock theory has limiting Einstein behavior.

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