Definition

Let (V,η)(V,\eta) be a finite-dimensional real Minkowski vector space, so η\eta has Lorentzian signature. Its Poincaré algebra is the semidirect-product

iso(V,η)=so(V,η)V,\mathfrak{iso}(V,\eta) =\mathfrak{so}(V,\eta)\ltimes V,

where the translation algebra VV is abelian and so(V,η)\mathfrak{so}(V,\eta) acts through its defining representation. Its bracket is

[(A,v),(B,w)]=([A,B],AwBv).[(A,v),(B,w)] =\bigl([A,B],Aw-Bv\bigr).

For four-dimensional , this is iso(1,3)\mathfrak{iso}(1,3), with dimension 6+4=106+4=10. It is the Lie algebra of the and of its identity component. Thus passing to the proper, orthochronous component does not change the Lie algebra.

For a nondegenerate form of arbitrary signature, the same semidirect-product formula defines the inhomogeneous orthogonal algebra iso(p,q)\mathfrak{iso}(p,q). The name “Poincaré algebra” is reserved here for Lorentzian signature.

Structure and extensions

The Lorentz algebra is a subalgebra and the translations form an abelian ideal. The quotient by translations is so(V,η)\mathfrak{so}(V,\eta). This semidirect structure is extended in the by odd supercharges whose bracket produces translations.

, internal RR-symmetries, and conformal extensions are additional structures, not part of the unextended Poincaré algebra.

References
  1. S. Weinberg, The Quantum Theory of Fields, Volume I: Foundations, Cambridge University Press, 1995. Publisher record. Relevant: Chapter 2.
  2. J. Figueroa-O'Farrill, “Classification of kinematical Lie algebras,” Journal of Mathematical Physics 59, 2018, 061701. Article.