Abstract

We propose a simple model of spacetime vacuum fluctuations motivated by AdS/CFT, where the vacuum is described by a thermal density matrix, ρ=e−KTr(e−K) with K the modular Hamiltonian. In AdS/CFT, both the expectation value of K and its fluctuations 〈ΔK2〉 have been calculated; both obey an area law identical to the Bekenstein-Hawking area law of black hole mechanics: 〈K〉=〈ΔK2〉=A4GN, where A is the area of an (extremal) entangling surface. It has also been shown that ΔK gravitates in AdS, and hence generates metric fluctuations. These theoretical results are intriguing, but it is not known how to precisely extend such ideas about holographic quantum gravity to ordinary flat space. We take the approach of considering whether experimental signatures in metric fluctuations could determine properties of the vacuum of quantum gravity in flat space. In particular, we propose a theoretical model motived by the AdS/CFT calculations that reproduces the most important features of modular Hamiltonian fluctuations; the model consists of a high occupation number bosonic degree of freedom. We show that if this theory couples through ordinary gravitational couplings to the mirrors in an interferometer with strain sensitivity similar to what will be available for gravitational waves, vacuum fluctuations could be observable.

Highlights

  • We propose a simple model of spacetime vacuum fluctuations motivated by AdS/CFT, where the vacuum is described by a thermal density matrix, ρ

  • We take the approach of considering whether experimental signatures in metric fluctuations could determine properties of the vacuum of quantum gravity in flat space

  • We show that if this theory couples through ordinary gravitational couplings to the mirrors in an interferometer with strain sensitivity similar to what will be available for gravitational waves, vacuum fluctuations could be observable

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Summary

On Vacuum Fluctuations in Quantum Gravity and Interferometer Arm Fluctuations

From the point of view of quantum mechanics and Effective Field Theory (EFT), these numbers represent the time and length scales of quantum fluctuations They are far out of reach of observational capabilities, and neatly encapsulate why the quantum effects of gravity have never been probed. Theoretical progress, mostly in the context of AdS/CFT and the black hole information paradox, suggests that non-locality and entanglement plays an important role in the quantum theory of gravity Holography, on the other hand, says that the degrees-of-freedom of a spacetime volume scales with the area of the surface bounding that volume As a result, this implies that QFT grossly overcounts the number of degrees-of-freedom when gravity is involved, suggesting that in any EFT description of spacetime, there should be long range correlations between the degrees-of-freedom. It is such long range correlations that we seek to model in this letter, where we call each spacetime degree-of-freedom a pixel

Our ability to quantify spacetime fluctuations from
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