Abstract
Erik Verlinde's theory of entropic gravity [arXiv:1001.0785], postulating that gravity is not a fundamental force but rather emerges thermodynamically, has garnered much attention as a possible resolution to the quantum gravity problem. Some have ruled this theory out on grounds that entropic forces are by nature noisy and entropic gravity would therefore display far more decoherence than is observed in ultra-cold neutron experiments. We address this criticism by modeling linear gravity acting on small objects as an open quantum system. In the strong coupling limit, when the model's unitless free parameter $\sigma$ goes to infinity, the entropic master equation recovers conservative gravity. We show that the proposed master equation is fully compatible with the \textit{q}\textsc{Bounce} experiment for ultra-cold neutrons as long as $\sigma\gtrsim 250$ at $90\%$ confidence. Furthermore, the entropic master equation predicts energy increase and decoherence on long time scales and for large masses, phenomena which tabletop experiments could test. In addition, comparing entropic gravity's energy increase to that of the Di\'{o}si-Penrose model for gravity induced decoherence indicates that the two theories are incompatible. These findings support the theory of entropic gravity, motivating future experimental and theoretical research.
Highlights
The theory of entropic gravity challenges the assumption that gravity is a conservative force, i.e., one that is proportional to the gradient of a potential energy
High Energy Phys. 04 (2011) 029], postulating that gravity is not a fundamental force but rather emerges thermodynamically, has garnered much attention as a possible resolution to the quantum gravity problem. Some have ruled this theory out on grounds that entropic forces are by nature noisy and entropic gravity would display far more decoherence than is observed in ultracold neutron experiments. We address this criticism by modeling linear gravity acting on small objects as an open quantum system
The definition of entropic forces follows from the first law of thermodynamics, δQ = dU + δW, which equates heat supplied to a system δQ to the change in the system’s internal energy dU plus work done δW
Summary
The theory of entropic gravity challenges the assumption that gravity is a conservative force, i.e., one that is proportional to the gradient of a potential energy. Newton’s second law F = ma immediately follows from the entropic force definition F = T S/ x after substituting (i) the amended form of Bekenstein’s formula S = 2π kb; (ii) the Compton wavelength x; and (iii) Unruh’s formula [3,4,5], kbT = ha/(2π c), connecting acceleration with temperature. Such a derivation of Newton’s second law is valid for a black hole—an extreme concentration of mass. A relationship to the Diósi-Penrose gravitational model is discussed
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