A Stern-Gerlach Experiment in Time

Abstract

In non-relativistic quantum mechanics, path integrals are normally derived from the Schroedinger equation. This assumes the two formalisms are equivalent. Since time plays a very different role in the Schroedinger equation and in path integrals, this may not be the case. We here derive path integrals directly by imposing two requirements: correct behavior in the classical limit and the most complete practicable symmetry between time and space. With these requirements, the path integral formalism predicts quantum fluctuations over the time dimension analogous to the quantum fluctuations seen over the three space dimensions. For constant potentials there is no effect. But the coupling between rapidly varying electromagnetic fields and the quantum fluctuations in time should be detectable. We consider a variation on the Stern-Gerlach experiment in which a particle with a non-zero electric dipole moment is sent through a rapidly varying electric field, oriented parallel to the particle's trajectory. The Schroedinger equation predicts changes to the precession frequency of the wave function about the trajectory but no physical splitting of the beam. With the approach here, path integrals predict the changes to the precession frequency and in addition that the beam will be split in velocity and time.

arXiv comment41 pages, 3 figures

References in corpus (6)

• Relativistic Nonlocality in experiments with successive impacts
• Does Quantum Mechanics imply influences acting backward in time in impact series experiments?
• Preferred Frame versus Multisimultaneity: meaning and relevance of a forthcoming experiment
• Quantum mechanical retrocausation? Call for nonlocal causal models!
• Uncollapsing the wave function
• Quantum mechanical 'Backward in Time'? Comments, Answers, and the Causal Indistinguishability Condition