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Simulating quantum field theory in curved spacetime with quantum many-body systems
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This paper proposes a new general framework to build a one-to-one correspondence between quantum field theories in static 1+1 dimensional curved spacetime and quantum many-body systems. We show that a massless scalar field in an arbitrary 2-dimensional static spacetime is always equivalent to a site-dependent bosonic hopping model, while a massless Dirac field is equivalent to a site-dependent free Hubbard model or a site-dependent isotropic XY model. A possible experimental realization for such a correspondence in trapped ions system is suggested. As applications of the analogue gravity model, we show that they can be used to simulate Hawking radiation of black hole and to study its entanglement. We also show in the analogue model that black holes are most chaotic systems and the fastest scramblers in nature. We also offer a concrete example about how to get some insights about quantum many-body systems from back hole physics.
Forward citations
Cited by 2 Pith papers
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Confinement Versus Screening in the Schwinger Model on AdS$_2$ from Bosonization and Tensor Networks
Massless QED2 on AdS2 is screened, not confined, when the static potential is defined after subtracting position-dependent probe self-energies.
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Simulating Hawking radiation in quantum many-body systems: deviations from the thermal spectrum
A bosonic hopping model that emulates quantum fields in curved spacetime is shown to reproduce the non-thermal E^2 corrections to Hawking radiation predicted by the tunneling method.
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