2016
DOI: 10.1088/1742-6596/701/1/012009
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Trading drift and fluctuations in entropic dynamics: quantum dynamics as an emergent universality class

Abstract: Abstract. Entropic Dynamics (ED) is a framework that allows the formulation of dynamical theories as an application of entropic methods of inference. In the generic application of ED to derive the Schrödinger equation for N particles the dynamics is a non-dissipative diffusion in which the system follows a "Brownian" trajectory with fluctuations superposed on a smooth drift. We show that there is a family of ED models that differ at the "microscopic" or sub-quantum level in that one can enhance or suppress the… Show more

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Cited by 12 publications
(24 citation statements)
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“…The transition probability-Next we maximize (1) subject to (5) and normalization. As discussed in [56] the multiplier α ′ associated to the global constraint (5) turns out to have no influence on the dynamics: it can be absorbed into the drift potential α ′ φ → φ which means we can effectively set α ′ = 1.…”
Section: The Entropic Dynamics Of Infinitesimal Stepsmentioning
confidence: 99%
“…The transition probability-Next we maximize (1) subject to (5) and normalization. As discussed in [56] the multiplier α ′ associated to the global constraint (5) turns out to have no influence on the dynamics: it can be absorbed into the drift potential α ′ φ → φ which means we can effectively set α ′ = 1.…”
Section: The Entropic Dynamics Of Infinitesimal Stepsmentioning
confidence: 99%
“…(2.12) for some integer n. For n = 0, the particles follow Brownian trajectories, which in the limit of η → 0 and ξ → 0 recovers the smooth Bohmian trajectories [12].…”
Section: The Transition Probabilitymentioning
confidence: 92%
“…The Lagrange multiplier α plays the role of controlling the relative strength of the fluctuations [12].…”
Section: The Transition Probabilitymentioning
confidence: 99%
“…As with any tool, its purpose is pragmatic in nature; that is, it is built to accomplish a particular 1 The Lagrange multiplier α ′ associated with the global constraint (3) turns out to be unimportant and can be chosen so that α ′ = 1. The interested reader can look to [19][20] for more information.…”
Section: Entropic Timementioning
confidence: 99%
“…This choice of dynamics has the added feature in that it singles out a preferred choice of representation for implementing path independence. That is, the generators G Ax appearing in (19) can be represented as Hamiltonian generators H Ax , with the brackets [ ·, · ] being identified with Poisson brackets. Naturally, a covariant dynamics for ρ and Φ can then be achieved by choosing the Hamiltonian generators that satisfy the algebra (19).…”
Section: Non-dissipative Covariant Dynamicsmentioning
confidence: 99%