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| | ON QUANTUM THEORETICAL ORIGINS OF NEWTONIAN TIME |
 | | The existence of a time operator, Fourier related to the energy of a "massless" oscillator clock, implies that cognate vectors symbolizing states in the standard quantum mechanics (QM) must generally be reinterpreted as processes, and that evolution of these processes must themselves be stochastic in the manner of a Feynman kernel. |
 | | All the G operators with aâ b, turn out to have extra factors of Δq(n), indicating that they will be made small relative to the a=b operators for very large n. |
 | | Nevertheless, for large, n, this last equation becomes the dynamical equation of QM for any energy operator E, where T is defined as the number operator in the basis that is the Υ transformed eigenbasis of E. The switch in sign of this commutator is consistent with what one would expect relativistically. |
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