Bounding the space of holographic CFTs with chaos

A bstract Thermal states of quantum systems with many degrees of freedom are subject to a bound on the rate of onset of chaos, including a bound on the Lyapunov exponent, λ L ≤ 2π/ β . We harness this bound to constrain the space of putative holographic CFTs and their would-be dual theories of AdS g...

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Bibliographic Details
Published inThe journal of high energy physics Vol. 2016; no. 10; pp. 1 - 60
Main Author Perlmutter, Eric
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.10.2016
Springer Nature B.V
Springer Berlin
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Summary:A bstract Thermal states of quantum systems with many degrees of freedom are subject to a bound on the rate of onset of chaos, including a bound on the Lyapunov exponent, λ L ≤ 2π/ β . We harness this bound to constrain the space of putative holographic CFTs and their would-be dual theories of AdS gravity. First, by studying out-of-time-order four-point functions, we discuss how λ L = 2π/ β in ordinary two-dimensional holographic CFTs is related to properties of the OPE at strong coupling. We then rule out the existence of unitary, sparse two-dimensional CFTs with large central charge and a set of higher spin currents of bounded spin; this implies the inconsistency of weakly coupled AdS 3 higher spin gravities without infinite towers of gauge fields, such as the SL( N ) theories. This fits naturally with the structure of higher-dimensional gravity, where finite towers of higher spin fields lead to acausality. On the other hand, unitary CFTs with classical W ∞ [ λ ] symmetry, dual to 3D Vasiliev or hs[ λ ] higher spin gravities, do not violate the chaos bound, instead exhibiting no chaos: λ L = 0. Independently, we show that such theories violate unitarity for | λ | > 2. These results encourage a tensionless string theory interpretation of the 3D Vasiliev theory.
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USDOE
FG02-91ER40671
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP10(2016)069