The Nilpotent Dirac Equation and its Applications in Particle Physics Peter Rowlands Department of Physics, University of Liverpool, Oliver Lodge Laboratory, Oxford Street, Liverpool, L69 7ZE, UK. e-mail
[email protected] Abstract. The nilpotent Dirac formalism has been shown, in previous publications, to generate new physical explanations for aspects of particle physics, with the additional possibility of calculating some of the parameters involved in the Standard Model. The applications so far obtained are summarised, with an outline of some more recent developments. 1 The nilpotent Dirac equation Some aspects of particle physics are more easily understood if we first express the Dirac equation in a more algebraic form than usual, with the gamma matrices replaced by equivalent operators from vector and quaternion algebra.1-7 Here, we define unit quaternion operators (1, i, j, k) according to the usual rules: i2 = j2 = k2 = ijk = −1 ij = −ji = k ; jk = −kj = i ; ki = −ik = j , and also multivariate 4-vector operators (i, i, j, k), which are isomorphic to complex quaternions or Pauli matrices: i2 = j2 = k2 = 1 ij = −ji = ik ; jk = −kj = ii ; ki = −ik = ij . The combination of these two sets of units produces a 32-part algebra (or group of order 64, taking into account both + and – signs), which can be directly related to that of the five γ matrices, with mappings of the form: γo = −ii ; γ1 = ik ; γ2 = jk ; γ3 = kk ; γ5 = ij , (1) or, alternatively, γo = ik ; γ1 = ii ; γ2 = ji ; γ3 = ki ; γ5 = ij . (2) Applying (1) directly to the conventional form of the Dirac equation, ∂ ∂ ∂ ∂ γ0 + γ1 + γ2 + γ3 + im ψ = 0 , ∂t ∂x ∂y ∂z 1 we obtain: ∂ ∂ ∂ ∂ −ii + ki + kj + kk + im ψ = 0 .