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From Poincaré to affine invariance: how does the Dirac equation generalize?

Ingo Kirsch1,3 and Djordje Sijacki2

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A generalization of the Dirac equation to the case of affine symmetry, with $\overline{SL}(4,\Bbb{R}$ replacing $\overline{SO}(1,3)$, is considered. A detailed analysis of a Dirac-type Poincaré-covariant equation for any spin j is carried out, and the related general interlocking scheme fulfilling all physical requirements is established. Embedding of the corresponding Lorentz fields into infinite-component $\overline{SL}(4,\Bbb{R}$ fermionic fields, the constraints on the $\overline{SL}(4,\Bbb{R}$ vector-operator generalizing Dirac's γ matrices, as well as the minimal coupling to (metric-)affine gravity are studied. Finally, a symmetry breaking scenario for $\overline{SA}(4,\Bbb{R}$ is presented which preserves the Poincaré symmetry.


PACS

03.65.Pm Relativistic wave equations

02.20.Qs General properties, structure, and representation of Lie groups

11.30.Qc Spontaneous and radiative symmetry breaking

11.30.Cp Lorentz and Poincare invariance

MSC

81T25 Quantum field theory on lattices

22E43 Structure and representation of the Lorentz group

81R40 Symmetry breaking

Subjects

Mathematical physics

Particle physics and field theory

Quantum information and quantum mechanics

Dates

Issue 12 (21 June 2002)

Received 4 December 2001

Published 27 May 2002



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