1. New Insights into Quantum Gravity from Holography Gary Horowitz UC Santa Barbara with N. Engelhardt (1509.07509, and in progress)

2. Happy Birthday David!

3. A powerful feature of gauge/gravity duality is that statements that are easy to establish on one side often imply highly nontrivial results about the dual theory. For example, the fact that black hole evaporation must be unitary follows immediately from unitary evolution of the dual gauge theory.

4. Assumptions: Gauge/gravity duality holds in a strong form: the two theories are equivalent at finite N and finite coupling. If a spacetime has several asymptotic regions, then each region is dual to a separate copy of the gauge theory. States may be entangled, but there is no coupling between the theories. The dual theory describes the spacetime inside black holes.

5. When can two QFTs communicate? Usually, two QFTs on separate spacetimes cannot send signals to one another QFT 1 QFT 2

6. Two copies of a CFT on Minkowski space can be mapped either to one static cylinder or two.

7. Definition: Two field theories are independent if the joint Hilbert space of the system can be written as a tensor product and all operators take the form No Transmission Principle (NTP): Two independent QFTs cannot transmit signals to one another. Application to holography: If two independent QFTs have gravity duals, then no signals can be transmitted between their bulk duals.

8. No evolution through black holes Could quantum gravity resolve the singularity and allow signals to emerge in another asymptotically AdS spacetime?

9. No evolution through black holes Could quantum gravity resolve the singularity and allow signals to emerge in another asymptotically AdS spacetime? No. The CFTs are independent, and this would violate the NTP.

10. A charged AdS black hole seems to violate the NTP even classically. But the inner horizon is known to be unstable. Signals cannot get through classically. NTP implies that signals cannot get through even in full quantum gravity.

11. Application to singular CFTs Some CFTs cannot be evolved past a certain time. If evolution on the boundary stops, then evolution in the bulk must stop as well. There must be a cosmological singularity classically, which quantum gravity cannot resolve into a bounce.

12. Consider CFTs on maximally conformally extended spacetimes. We assume the spacetime is topologically S x R, where S is compact, and can be foliated by a one parameter family of Cauchy surfaces S t. Definition: A standard conformal frame is one in which the volume of S t is bounded from above and below by nonzero constants for all t. Definition: A CFT is singular if evolution ends in finite time in a standard conformal frame. What is a singular CFT?

13. Examples of singular CFTs 1)Put any CFT on a spacetime with a cosmological singularity, e.g., If Σ p i = 0, this is in a standard conformal frame. (Das, Michelson, Narayan, Trivedi; Engelhardt, Hertog, G.H.) 2)Destabilize a CFT by adding a potential unbounded from below, e.g., (Hertog, G.H.; Craps, Hertog, Turok; Barbon, Rabinovici) 3)Add a relevant perturbation to a CFT on de Sitter (Maldacena; Harlow, Susskind; Barbon, Rabinovici)

14. Classical SUGRA implications In all 3 cases, there are bulk solutions with cosmological singularities. The NTP implies this must always be the case. Not allowed

15. If the boundary metric has a cosmological singularity, we get a purely geometric result which is like a new type of singularity theorem: If the conformal boundary metric of an asymptotically AdS solution of low energy string theory has a cosmological singularity, then the bulk solution must also have a cosmological singularity. This is not obvious. There are nonsingular bulk metrics with singular boundary metrics:

16. Classical string theory implications Consider a Lorentzian cone ds 2 = - dτ 2 + τ 2 dx 2 where x is periodically identified with period x 0. With antiperiodic boundary conditions for fermions, closed string winding modes become tachyonic when |τ| x 0 ~ L s. Spacetime ends when the tachyon condenses (McGreevy and Silverstein). Can signals pass through a tachyon condensate?

17. No. Consider AdS 3 in Poincare coordinates ds 2 = [- dτ 2 + τ 2 dx 2 + dz 2 ] / z 2 Tachyons condense when |τ| x 0 / z < L s In a standard conformal frame, each light cone is conformal to an infinite cylinder. So no signals can get through the bulk.

18. Quantum gravity implications Cosmological singularities associated with singular CFTs cannot be resolved into quantum bounces. But: Can holography fail since there are large quantum gravity effects which extend out to infinity? Could this cause the boundary metric to fluctuate? In Fefferman-Graham gauge, the boundary metric must be singular for any bulk with large asymptotic curvature. The curvature of is R = (const) + z 2 R 0

19. Quantum effects are expected to be significant within a bounded distance to the singularity. Suppose the singularity is at t = 0 and quantum effects are important for |t| < t 0. Due to the conformal rescaling, all these effects are shrunk to zero proper time in the boundary metric. Quantum gravity fluctuations do not affect the boundary metric away from the singularity. Note: Any regularization of the CFT singularity turns the bulk cosmological singularity into a black hole:

20. Our conclusion about no quantum bounces only applies to cosmological singularities in holography. It does not rule out bounces based on T-duality or colliding branes, or in other approaches to quantum gravity such as loop quantum gravity.

21. A possible holographic bounce? (Awad, Das, Nampuri, Narayan, Trivedi) Consider N = 4 SYM on Minkowski space with coupling g YM (t) that vanishes at t = 0. Since g YM 2 = e φ the dilaton diverges in the bulk. Find BUT: SYM does not become free near t = 0. There is strong evidence that evolution must end, since the state becomes singular with diverging energy as t - > 0.

22. Comments 1)One cannot avoid our conclusions by adding couplings between the CFTs associated with different asymptotic regions, since that would violate causality. 1)One could make up a rule to identify a state in CFT 1 with one in CFT 2, but it would be extra input not contained in the original CFTs – bulk and boundary theories would not be equivalent. 1)There is no natural way to identify the states.

23. 4)If the CFT does not describe the region inside the horizon, we cannot rule out the possibility that QG allows signals to propagate through a singularity to a region inside another horizon.

24. Cosmic censorship Classical GR conjecture: Generic, asymptotically flat, initial data has a maximal evolution that contains a complete null infinity. Initial data i.e. this can’t happen. I+I+ If cosmic censorship fails, it was hoped that quantum gravity would provide boundary conditions, so evolution continues.

25. In holography we know that this is true! Regardless of what happens in a localized region in the interior, evolution in the CFT on the boundary continues. ? QGCFT

26. Summary A number of nontrivial statements follow from simple assumptions about holography including: 1)Cannot evolve through black holes to another asymptotically AdS region of spacetime. 2)Cannot evolve through certain cosmological singularities to another region of spacetime. 3)A form of cosmic censorship holds in QG.

27. Happy Birthday David!