Duffin–Kemmer–Petiau algebra

In mathematical physics, the Duffin–Kemmer–Petiau algebra (DKP algebra), introduced by R.J. Duffin, Nicholas Kemmer and G. Petiau, is the algebra which is generated by the Duffin–Kemmer–Petiau matrices. These matrices form part of the Duffin–Kemmer–Petiau equation that provides a relativistic description of spin-0 and spin-1 particles.

The DKP algebra is also referred to as the meson algebra.^[1]

Defining relations

The Duffin–Kemmer–Petiau matrices have the defining relation^[2]

${\displaystyle \beta ^{a}\beta ^{b}\beta ^{c}+\beta ^{c}\beta ^{b}\beta ^{a}=\beta ^{a}\eta ^{bc}+\beta ^{c}\eta ^{ba}}$

where ${\displaystyle \eta ^{ab}}$ stand for a constant diagonal matrix. The Duffin–Kemmer–Petiau matrices ${\displaystyle \beta }$ for which ${\displaystyle \eta ^{ab}}$ consists in diagonal elements (+1,-1,...,-1) form part of the Duffin–Kemmer–Petiau equation. Five-dimensional DKP matrices can be represented as:^[3][4]

${\displaystyle \beta ^{0}={\begin{pmatrix}0&1&0&0&0\\1&0&0&0&0\\0&0&0&0&0\\0&0&0&0&0\\0&0&0&0&0\end{pmatrix}}}$, ${\displaystyle \quad \beta ^{1}={\begin{pmatrix}0&0&-1&0&0\\0&0&0&0&0\\1&0&0&0&0\\0&0&0&0&0\\0&0&0&0&0\end{pmatrix}}}$, ${\displaystyle \quad \beta ^{2}={\begin{pmatrix}0&0&0&-1&0\\0&0&0&0&0\\0&0&0&0&0\\1&0&0&0&0\\0&0&0&0&0\end{pmatrix}}}$, ${\displaystyle \quad \beta ^{3}={\begin{pmatrix}0&0&0&0&-1\\0&0&0&0&0\\0&0&0&0&0\\0&0&0&0&0\\1&0&0&0&0\end{pmatrix}}}$

These five-dimensional DKP matrices represent spin-0 particles. The DKP matrices for spin-1 particles are 10-dimensional.^[3] 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.^[5]

Duffin–Kemmer–Petiau equation

The Duffin–Kemmer–Petiau equation (DKP equation, also: Kemmer equation) is a

${\displaystyle (i\hbar \beta ^{a}\partial _{a}-mc)\psi =0}$

where ${\displaystyle \beta ^{a}}$ are Duffin–Kemmer–Petiau matrices, ${\displaystyle m}$ is the particle's mass, ${\displaystyle \psi }$ its

, ${\displaystyle \hbar }$ the reduced Planck constant, ${\displaystyle c}$ the speed of light. For massless particles, the term ${\displaystyle mc}$ is replaced by a singular matrix ${\displaystyle \gamma }$ that obeys the relations ${\displaystyle \beta ^{a}\gamma +\gamma \beta ^{a}=\beta ^{a}}$ and ${\displaystyle \gamma ^{2}=\gamma }$.

The DKP equation for spin-0 is closely linked to the Klein–Gordon equation^[4][6] and the equation for spin-1 to the Proca equations.^[7] It suffers the same drawback as the Klein–Gordon equation in that it calls for negative probabilities.^[4] Also the De Donder–Weyl covariant Hamiltonian field equations can be formulated in terms of DKP matrices.^[8]

History

The Duffin–Kemmer–Petiau algebra was introduced in the 1930s by R.J. Duffin,^[9] N. Kemmer^[10] and G. Petiau.^[11]

Further reading

• Fernandes, M. C. B.; Vianna, J. D. M. (1999). "On the generalized phase space approach to Duffin–Kemmer–Petiau particles". Foundations of Physics. 29 (2). Springer Science and Business Media LLC: 201–219.
  S2CID 118277218
  .
• Fernandes, Marco Cezar B.; Vianna, J. David M. (1998). "On the Duffin-Kemmer-Petiau algebra and the generalized phase space". Brazilian Journal of Physics. 28 (4). FapUNIFESP (SciELO): 00.
  ISSN 0103-9733
  .
• Sharp, Robert T.; Winternitz, Pavel (2004). "Bhabha and Duffin–Kemmer–Petiau equations: spin zero and spin one". Symmetry in physics : in memory of Robert T. Sharp. Providence, R.I.: American Mathematical Society. p. 50 ff.
  OCLC 53953715
  .
• Fainberg, V.Ya.; Pimentel, B.M. (2000). "Duffin–Kemmer–Petiau and Klein–Gordon–Fock equations for electromagnetic, Yang–Mills and external gravitational field interactions: proof of equivalence". Physics Letters A. 271 (1–2). Elsevier BV: 16–25.
  S2CID 9595290
  .

References