Abstract
This paper provides a rigorous mathematical derivation of Paul Dirac’s relativistic wave equation, tracing its theoretical evolution from fundamental spacetime differential operators to manifestly covariant quantum mechanical expressions. Beginning with the four-gradient operator in Minkowski space, it examines the foundational non-relativistic Schrödinger mechanics, highlighting the geometric and physical limitations of the second-order Klein-Gordon theory. It demonstrates how Dirac’s first-order Hamiltonian ansatz overcomes negative probability density issues through matrix-valued coefficients. By detailing the explicit 4 x 4 matrix representations, commutation constraints, and Clifford algebra structure satisfied by the Dirac gamma matrices, it showcases the complete transition from non-relativistic Schrödinger mechanics to a fully Lorentz-covariant formulation.



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