Entanglement and the Bekenstein-Hawking entropy

Transcription

1 Entanglement and the Bekenstein-Hawking entropy Eugenio Bianchi relativity.phys.lsu.edu/ilqgs International Loop Quantum Gravity Seminar

2 Black hole entropy Bekenstein-Hawking 1974 Process: matter falling in area increases Entropy change Puzzle: the entropy of what? 2

3 Vacuum entanglement in QFT Sorkin 1983 Vacuum state on Minkowski space Reduced density matrix Entropy due to correlations at space-like separations Divergent: introduce UV cut-off Related to BH entropy? Problems: - - species New result: in low-energy processes arxiv: = finite and universal = 3

4 The Horizon of a black hole - Equivalence Principle - Causal horizon Horizon radius: Minkowski space-time at scales Curvature at the horizon: 4

5 Plan of the talk Entanglement and the Bekenstein-Hawking entropy: arxiv: [gr-qc] I. Perturbative quantum gravity II. The perturbed Rindler horizon III. Entanglement and thermality IV. Area law for entanglement perturbations 5

6 I. Perturbative quantum gravity - Minkowski space-time - Graviton field - Action: (Einstein-Hilbert + matter; perturbative) E.O.M. (*) (Harmonic gauge ) Energy-momentum tensor gravitons matter 6

7 Entanglement and gravity I. Perturbative quantum gravity (*) II. The perturbed Rindler horizon III. Entanglement and thermality of the vacuum IV. Area law for entanglement perturbations 7

8 II. The Rindler horizon Minkowski space-time Cartesian coord. Rindler coord. Metric Accelerated observer at : proper time, acceleration Rindler Horizon : light-like surface with 8

9 II. The perturbed Rindler horizon - Collimated beam of light rays - Energy crossing the beam Gravity is attractive: it focuses light rays Perturbatively: interaction In GR: curvature with light rays geodesic deviation expansion, Raychaudhuri eq. 9

10 II. The perturbed Rindler horizon Event horizon: Light rays finely balanced between out of sight reach infinity Gravity is attractive: it focuses light rays diverging beam so that collimated at infinity Area increase: 10

11 Entanglement and gravity I. Perturbative quantum gravity (*) II. The perturbed Rindler horizon (**) III. Entanglement and thermality of the vacuum IV. Area law for entanglement perturbations 11

12 II. Rindler energy Rindler energy: = boost Killing vector (** * ) Energy flux through the horizon, 12

13 Entanglement and gravity I. Perturbative quantum gravity (*) II. The perturbed Rindler horizon (**) (** * ) III. Entanglement and thermality of the vacuum IV. Area law for entanglement perturbations 13

14 III. Entanglement and thermality of the vacuum Free field, Minkowski vacuum Minkowski vacuum, interacting QFT, Reduced density matrix: Gibbs state at temperature 14

15 Entanglement and gravity I. Perturbative quantum gravity (*) II. The perturbed Rindler horizon (**) (** * ) III. Entanglement and thermality of the vacuum ( * * * ) IV. Area law for entanglement perturbations 15

16 IV. Entanglement perturbations and universality Entanglement entropy of the vacuum If you can t change anything, you are not doing thermodynamics 16

17 IV. Low-energy perturbation of the vacuum Excited state, Entanglement entropy perturbation, ( * * * ) (** * ) (*) (**) 17

18 Entanglement and gravity I. Perturbative quantum gravity (*) II. The perturbed Rindler horizon (**) (** * ) III. Entanglement and thermality of the vacuum ( * * * ) IV. Area law for entanglement perturbations 18

19 Why are black holes hot? 19

20 Why are black holes hot? because of entanglement across the horizon 20

21 Why are black holes hot? because of entanglement across the horizon 21

22 Why are black holes hot? because of entanglement across the horizon 22

23 Relevance to Loop Quantum Gravity: I In the spin-foam calculation of black-hole entropy arxiv: entanglement and the boost Hamiltonian ilqgs/bianchi pdf - relation to the thermal ensemble picture ( ABCK, ENP, ilqgs/perez pdf ) 23

24 Relevance to Loop Quantum Gravity: II Entanglement entropy of spin-network states ( W. Donnelly, , ) On the architecture of spacetime geometry [hep-th] with R. Myers Conjecture: In a theory of quantum gravity, - for every large region - and smooth spacetime Entanglement entropy of a spin-network as a probe of semiclassicality 24