One-to-one correspondence between entanglement mechanics and black hole
thermodynamics
- URL: http://arxiv.org/abs/2010.03418v1
- Date: Wed, 7 Oct 2020 13:57:57 GMT
- Title: One-to-one correspondence between entanglement mechanics and black hole
thermodynamics
- Authors: S. Mahesh Chandran, S. Shankaranarayanan (IIT Bombay)
- Abstract summary: We establish a one-to-one mapping between entanglement entropy, energy, and temperature.
We show this universally for 4-D spherically symmetrically flat and non-flat space-times with single and multiple horizons.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We establish a one-to-one mapping between entanglement entropy, energy, and
temperature (quantum entanglement mechanics) with black hole entropy, Komar
energy, and Hawking temperature, respectively. We show this explicitly for 4-D
spherically symmetric asymptotically flat and non-flat space-times with single
and multiple horizons. We exploit an inherent scaling symmetry of entanglement
entropy and identify scaling transformations that generate an infinite number
of systems with the same entanglement entropy, distinguished only by their
respective energies and temperatures. We show that this scaling symmetry is
present in most well-known systems starting from the two-coupled harmonic
oscillator to quantum scalar fields in spherically symmetric space-time. The
scaling symmetry allows us to identify the cause of divergence of entanglement
entropy to the generation of (near) zero-modes in the systems. We
systematically isolate the zero-mode contributions using suitable boundary
conditions. We show that the entanglement entropy and energy of quantum scalar
field scale differently in space-times with horizons and flat space-time. The
relation $E=2TS$, in analogy with the horizon's thermodynamic structure, is
also found to be universally satisfied in the entanglement picture. We then
show that there exists a one-to-one correspondence leading to the Smarr-formula
of black hole thermodynamics for asymptotically flat and non-flat space-times.
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