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Research Article Open access CC BY 4.0

On Representations of the Lorentz Group

Paul R. Gerber

Journal of Advances in Mathematics and Computer Science · pp. 76–82 · Published 28 Apr 2023

10.9734/jamcs/2023/v38i71774

Abstract

The Lorentz group is a non-compact group. Consequently, it's representations cannot be expected to be equivalent to representations of a unitary group. Actually, they act on a large-component space and a separated small-component space, in some sense analogous to 4-vectors. In contrast to representations of compact groups state vectors carry the actual value of the non-compact variables, the boost-vector. In the non-boosted state the small components vanish and the large components transform according to a representation of the rotation subgroup. Application of a boost then generates small components, a process that preserves norms. However, the norm now has a growing positive contribution from the large-components and a negative contribution from the small-components, growing absolutely to keep the total unchanged. General transformations are described in detail. The freedom to assign boost directions to the phases of small components leads to a topological symmetry with avor-generating representations for two sheeted representations.

Special relativity Lorentz group non-unitarity representation quantum mechanics field theory elementary particles flavor

References (8)

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  2. 2 The Classical Theory of Fields [DOI]
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  5. 5 On Unitary Representations of the Inhomogeneous Lorentz Group [DOI]
  6. 6 Introduction to Elementary Particles 3 [DOI]
  7. 7 On Quantum Field Theory and Gravitation
  8. 8 On Generations in Elementary Particle Physics

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