Poincare and Heisenberg quantum dynamical symmetry: Casimir invariant field equations of the quaplectic group
Stephen G. Low

TL;DR
This paper explores the role of the quaplectic group, combining Poincare and Heisenberg symmetries, in deriving quantum field equations through Casimir invariants, extending the understanding of symmetries in quantum physics.
Contribution
It introduces the quaplectic group as a unified symmetry framework and derives general field equations using Mackey representation theory.
Findings
Derived field equations from the Casimir invariants of the quaplectic group.
Showed the quaplectic group contains multiple Poincare subgroups and the Heisenberg group.
Extended the symmetry-based derivation of quantum field equations beyond the Poincare group.
Abstract
The unitary irreducible representations of a Lie group defines the Hilbert space on which the representations act. If this Lie group is a physical quantum dynamical symmetry group, this Hilbert space is identified with the physical quantum state space. The eigenvalue equations for the representation of the set of Casimir invariant operators define the field equations of the system. The Poincare group is the archetypical example with the unitary representations defining the Hilbert space of relativistic particle states and the Klein-Gordon, Dirac, Maxwell equations are obtained from the representations of the Casimir invariant operators eigenvalue equations. The representation of the Heisenberg group does not appear in this derivation. The unitary representations of the Heisenberg group, however, play a fundamental role in nonrelativistic quantum mechanics, defining the Hilbert space and…
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Taxonomy
TopicsNonlinear Waves and Solitons · Nonlinear Photonic Systems · Mechanical and Optical Resonators
