The Bekenstein Bound
Abstract
Bekenstein's conjectured entropy bound for a system of linear size R and energy E, namely S ≤ 2 π E R, has counterexamples for many of the ways in which the "system," R, E, and S may be defined. One consistent set of definitions for these quantities in flat Minkowski spacetime is that S is the total von Neumann entropy and E is the expectation value of the energy in a "vacuum-outside-R" quantum state that has the the vacuum expectation values for all operators entirely outside a sphere of radius R. However, there are counterexamples to the Bekenstein bound for this set of definitions. Nevertheless, an alternative formulation ten years ago by Horacio Casini for the definitions of S and of 2 π E R have finally enabled a proof for this particular formulation of the Bekenstein bound.
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