Abstract

We evaluate the full time dependence of holographic complexity in various eternal black hole backgrounds using both the complexity=action (CA) and the complexity=volume (CV) conjectures. We conclude using the CV conjecture that the rate of change of complexity is a monotonically increasing function of time, which saturates from below to a positive constant in the late time limit. Using the CA conjecture for uncharged black holes, the holographic complexity remains constant for an initial period, then briefly decreases but quickly begins to increase. As observed previously, at late times, the rate of growth of the complexity approaches a constant, which may be associated with Lloyd’s bound on the rate of computation. However, we find that this late time limit is approached from above, thus violating the bound. For either conjecture, we find that the late time limit for the rate of change of complexity is saturated at times of the order of the inverse temperature. Adding a charge to the eternal black holes washes out the early time behaviour, i.e. complexity immediately begins increasing with sufficient charge, but the late time behaviour is essentially the same as in the neutral case. We also evaluate the complexity of formation for charged black holes and find that it is divergent for extremal black holes, implying that the states at finite chemical potential and zero temperature are infinitely more complex than their finite temperature counterparts.

Highlights

  • In recent years, surprising new connections have been developing between quantum information and quantum gravity

  • We investigate the properties of complexity for charged black holes

  • We find that the holographic complexity smoothly approaches to that of the neutral black holes in the limit of zero charge

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Summary

Introduction

In recent years, surprising new connections have been developing between quantum information and quantum gravity. A prime arena for discussions of holographic complexity has been the eternal two-sided black hole and this will be the case in the present paper This bulk geometry is dual to the thermofield double state in the boundary theory [21], TFD(tL, tR) = Z−1/2 e−Eα/(2T ) e−iEα(tL+tR) Eα L Eα R , α (1.1). We find that the rate of change of complexity approaches its late time limit with an exponential decay where the characteristic time scale is proportional to the inverse temperature For both conjectures (and in d ≥ 3), we examined the rate of change of complexity for charged black holes, as well as their complexity of formation. We study the time evolution of holographic complexity using the complexity=action (CA) conjecture [8, 9] for (neutral) eternal AdS black holes in d + 1 dimensions.

Evaluating the action
Time dependence of complexity
Comments
Examples
BTZ black holes
Late time behaviour
General time dependence
Charged black holes
Discussion
General boundary times
Boundary counterterm
B Additional examples of time dependence of complexity
C Late time behaviour for the CV proposal
D Complexity of formation for charged black holes
Small hyperbolic black holes
E Ambiguities in the action calculations

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