Null states and time evolution in a toy model of black hole dynamics

May 7, 2024
30 pages
Published in:
  • JHEP 08 (2024) 199
  • Published: Aug 23, 2024
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Abstract: (Springer)
Spacetime wormholes can provide non-perturbative contributions to the gravitational path integral that make the actual number of states eS^{S} in a gravitational system much smaller than the number of states eSp {e}^{S_{\textrm{p}}} predicted by perturbative semiclassical effective field theory. The effects on the physics of the system are naturally profound in contexts in which the perturbative description actively involves N = O(eS^{S}) of the possible eSp {e}^{S_{\textrm{p}}} perturbative states; e.g., in late stages of black hole evaporation. Such contexts are typically associated with the existence of non-trivial quantum extremal surfaces. However, by forcing a simple topological gravity model to evolve in time, we find that such effects can also have large impact for N ≪ eS^{S} (in which case no quantum extremal surfaces can arise). In particular, even for small N, the insertion of generic operators into the path integral can cause the non-perturbative time evolution to differ dramatically from perturbative expectations. On the other hand, this discrepancy is small for the special case where the inserted operators are non-trivial only in a subspace of dimension D ≪ eS^{S}. We thus study this latter case in detail. We also discuss potential implications for more realistic gravitational systems.
Note:
  • 30 pages, 11 figures
  • AdS-CFT Correspondence
  • Black Holes
  • Models of Quantum Gravity
  • gravitation: model
  • gravitation: path integral
  • space-time: wormhole
  • black hole: evaporation
  • gravitation: topological
  • nonperturbative
  • surface