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Quantum Mechanics with Horizons Stefan Leichenauer Caltech (soon - PowerPoint PPT Presentation

Quantum Mechanics with Horizons Stefan Leichenauer Caltech (soon UC Berkeley) Outline Quantum Mechanics Black Hole Puzzles Cosmology Puzzles Lessons from AdS/CFT Fleshing out a thought experiment Quantum Mechanics The


  1. Quantum Mechanics with Horizons Stefan Leichenauer Caltech (soon UC Berkeley)

  2. Outline • Quantum Mechanics • Black Hole Puzzles • Cosmology Puzzles • Lessons from AdS/CFT • Fleshing out a thought experiment…

  3. Quantum Mechanics • The role of the observer is very important. • Super-observer: exists outside of the system, can choose to “observe” and sees Born Rule probabilities. • Observer within the system: large? classical? lives on a branch? makes records? • The super-observer can ask questions about the observer. Proceeding without the super-observer perspective is difficult/controversial.

  4. Black Hole Puzzles • Hawking calculation: information paradox. non- unitarity? large deviations from EFT? • Apparent quantum cloning: both the infalling matter and the Hawking radiation on the same slice. Inconsistency of the global super-observer perspective.

  5. Black Hole Puzzles • Solution(?): Complementarity. The global super-observer perspective is unphysical: no observer within the system can probe both inside and outside.

  6. Cosmology Puzzles • Horizons also occur in de Sitter space. • Difference between BH and dS horizons: dS horizons do not evaporate, no information paradox.

  7. Cosmology Puzzles • Puzzle: Landscape + dS = Multiverse and the measure problem • Complementarity: the lesson from black holes is that QG wants to be a theory of one causal patch (at a time?). Helps with measure problem.

  8. AdS/CFT • Quantum field theory on the boundary = quantum gravity in the bulk • Local operators in field theory = operators at infinity in the bulk • To probe deep inside the bulk, must look at something nonlocal in the field theory.

  9. Lessons from AdS/CFT • This is QG, we just need to understand it. There is only a partial understanding of the dictionary. • This is a super-observer theory, complete with Hilbert space and wavefunction. We can put the universe in a lab. • Can we see complementarity? How do we go inside the horizon?

  10. Black Holes in AdS/CFT • Thermofield double state in CFTxCFT. • Outside of the horizon: no problem. • Behind the horizon??? (some entanglement calculations make use of the behind-the-horizon region)

  11. A thought experiment… • Alice and Bob jump into opposite sides of the eternal AdS black hole. Do they meet? • There is no interaction between the two CFTs. Contrast with two people meeting in the middle of a room. • How can we track the degrees of freedom of Alice and Bob as they cross the horizon? Can the region behind the horizon be made of entanglements of two CFTs? • Toy model or no-go theorem would be nice!

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