Hydrodynamics of spacetime and vacuum viscosity
Christopher Eling

TL;DR
This paper reformulates the derivation of Einstein's equations using hydrodynamics, showing that vacuum spacetime behaves like a fluid with a shear viscosity to entropy density ratio of /4, linking gravity, thermodynamics, and quantum theory.
Contribution
It introduces a hydrodynamic perspective to vacuum spacetime, deriving Einstein's equations from horizon fluid dynamics and identifying the shear viscosity to entropy density ratio as /4.
Findings
Vacuum thermal state obeys hydrodynamic equations.
Einstein's equations emerge from horizon fluid dynamics.
Shear viscosity to entropy density ratio is /4, consistent with gauge/gravity duality.
Abstract
It has recently been shown that the Einstein equation can be derived by demanding a non-equilibrium entropy balance law dS = dQ/T + dS_i hold for all local acceleration horizons through each point in spacetime. The entropy change dS is proportional to the change in horizon area while dQ and T are the energy flux across the horizon and Unruh temperature seen by an accelerating observer just inside the horizon. The internal entropy production term dS_i is proportional to the squared shear of the horizon and the ratio of the proportionality constant to the area entropy density is \hbar/4\pi. Here we will show that this derivation can be reformulated in the language of hydrodynamics. We postulate that the vacuum thermal state in the Rindler wedge of spacetime obeys the holographic principle. Hydrodynamic perturbations of this state exist and are manifested in the dynamics of a stretched…
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