Abstract

The concept of time emerges as an ordering structure in a classical statistical ensemble. Probability distributions pτ(t)p_τ(t) at a given time tt obtain by integrating out the past and future. We discuss all-time probability distributions that realize a unitary time evolution as described by rotations of the real wave function qτ(t)=±pτ(t)q_τ(t)=\pm \sqrt{p_τ(t)}. We establish a map to quantum physics and the Schrödinger equation. Suitable classical observables are mapped to quantum operators. The non-commutativity of the operator product is traced back to the incomplete statistics of the local-time subsystem. Our investigation of classical statistics is based on two-level observables that take the values one or zero. Then the wave functions can be mapped to elements of a Grassmann algebra. Quantum field theories for fermions arise naturally from our formulation of probabilistic time.

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