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The quaternionic commutator bracket and its implications

Abstract

A quaternionic commutator bracket for position and momentum shows that the quaternionic wave function, \emph{viz.} ψ~=(icβ€‰Οˆ0 ,Οˆβƒ—)\widetilde{\psi}=(\frac{i}{c}\,\psi_0\,,\vec{\psi}), represents a state of a particle with orbital angular momentum, L=3 ℏL=3\,\hbar, resulting from the internal structure of the particle. This angular momentum can be attributed to spin of the particle. The vector Οˆβƒ—\vec{\psi}, points along the direction of Lβƒ—\vec{L}. When a charged particle is placed in an electromagnetic fields the interaction energy reveals that the magnetic moments interact with the electric and magnetic fields giving rise to terms similar to Aharonov-Bohm and Aharonov-Casher effects.Comment: 8 page

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