Bounding the Space of Holographic CFTs with Chaos

Feb 26, 2016
66 pages
Published in:
  • JHEP 10 (2016) 069
  • Published: Oct 13, 2016
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Abstract: (Springer)
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, λL_{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 λL_{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 AdS3_{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: λL_{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.
Note:
  • 50+18 pages. v3: Section 3 clarified and reorganized, related improvements
  • AdS-CFT Correspondence
  • Conformal and W Symmetry
  • Higher Spin Gravity
  • field theory: conformal
  • spin: high
  • gravitation: higher-dimensional
  • n-point function: 4
  • duality: holography
  • operator product expansion
  • Lyapunov exponent