1999Journal of Physics A Mathematical and GeneralOpen access

Representations of the discrete inhomogeneous Lorentz group and Dirac wave equation on the lattice

Miguel Lorente, Peter Krämer

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Abstract

We propose the fundamental and two-dimensional representation of the Lorentz groups on a (3+1)-dimensional hypercubic lattice, from which representations of higher dimensions can be constructed. For the unitary representation of the discrete translation group we use the kernel of the Fourier transform. From the Dirac representation of the Lorentz group (including reflections) we derive in a natural way the wave equation on the lattice for spin-1/2 particles. Finally, the induced representation of the discrete inhomogeneous Lorentz group is constructed by standard methods and its connection with the continuous case is discussed.

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We propose the fundamental and two-dimensional representation of the Lorentz groups on a (3+1)-dimensional hypercubic lattice, from which representations of higher dimensions can be constructed. For the unitary representation of the discrete translation group we use the kernel of the Fourier transform. From the Dirac representation of the Lorentz group (including reflections) we derive in a natural way the wave equation on the lattice for spin-1/2 particles. Finally, the induced representation of the discrete inhomogeneous Lorentz group is constructed by standard methods and its connection with the continuous case is discussed.

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Available abstract

We propose the fundamental and two-dimensional representation of the Lorentz groups on a (3+1)-dimensional hypercubic lattice, from which representations of higher dimensions can be constructed. For the unitary representation of the discrete translation group we use the kernel of the Fourier transform. From the Dirac representation of the Lorentz group (including reflections) we derive in a natural way the wave equation on the lattice for spin-1/2 particles. Finally, the induced representation of the discrete inhomogeneous Lorentz group is constructed by standard methods and its connection with the continuous case is discussed.

Key concepts: Lorentz group, Unitary representation, Representation theory of the Lorentz group, Lorentz transformation, Group representation, Lattice (music), Bispinor, Irreducible representation

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