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Using the language of the Geometric Algebra, we recast the massive Diracbispinor as a set of Lorentz scalar, vector, bivector, pseudovector, andpseudoscalar fields that obey a generalized form of Maxwell's equations ofelectromagnetism. This field-based formulation requires careful distinctionbetween geometric and non-geometric implementations of the imaginary unitscalar in the Dirac algebra. This distinction, which is obscured inconventional treatments, allows us to find alternative constructions of thefield bilinears and a more natural interpretation of the discrete C, P, and Ttransformations.

On the Physical Interpretation of the Dirac Wavefunction II: The Massive Dirac Field