Duffin–Kemmer–Petiau algebra

Duffin–Kemmer–Petiau algebra

In mathematical physics, the Duffin–Kemmer–Petiau algebra (DKP algebra) is the algebra which is generated the Duffin–Kemmer–Petiau matrices, introduced by Duffin, Kemmer and Petiau.

These matrices have the defining relation[1]

βμβνβα + βαβνβμ = gμνβα + gαμβν

where gμν is the Galilean metric, represented by the Kronecker symbol gμν = δμν.

The Duffin–Kemmer–Petiau matrices form part of the Duffin–Kemmer–Petiau equation, which describes spin-0 and spin-1 particles in the description of the standard model and is closely linked to the Proca equations[1] and the Klein–Gordon equation.[2] The Duffin–Kemmer–Petiau equation suffers the same drawback as the Klein–Gordon equation in that it calls for negative probabilities.[2]

The DKP-algebra can be reduced to a direct sum of irreducible subalgebras for spin‐0 and spin‐1 bosons, the subalgebras being defined by multiplication rules for the linearly independent basis elements.[3]

It has been shown that the equation is closely linked to the De Donder–Weyl covariant Hamiltonian field equations.[4]

Further reading

References

  1. ^ a b Sergey Kruglov: Symmetry and electromagnetic interaction of fields with multi-spin. A Volume in Contemporary Fundamental Physics, ISBN 1-56072-880-9, 2000, p. 26
  2. ^ a b Anton Z. Capri: Relativistic quantum mechanics and introduction to quantum field theory, World Scientific, 2002, ISBN 981-238-136-8, p. 25
  3. ^ Ephraim Fischbach, Michael Martin Nieto, C. K. Scott: Duffin‐Kemmer‐Petiau subalgebras: Representations and applications, Journal of Mathematical Physics, vol. 14, no. 12, 1760 (1973), DOI: 10.1063/1.1666249 (abstract)
  4. ^ Igor V. Kanatchikov: On the Duffin–Kemmer–Petiau formulation of the covariant Hamiltonian dynamics in field theory, hep-th/9911/9911175v1 (submitted 23. November 1999)