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A fully relativistic (Lorentz covariant) description, first put forward by Paul Dirac in 1928, of the first quantized, spin one half fermion with nonzero mass. Physical notions to do with this equation include the Dirac sea, Dirac hole theory, the Klein Paradox and the fine structure of the Hydrogen spectrum.
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Lorentz transformation and causality of the Dirac field
Consider the Dirac quantum field $$\psi(x) = \int \frac{d^{3}p}{(2\pi)^3} \frac{1}{\sqrt{2E_{\mathbb{p}}}} \sum_{s} [a^{s}_{\mathbb{p}}u^{s}(\mathbb{p})e^{-\mathrm{i}p \cdot x} + b^{s\dagger}_{\mathbb …
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Wrong sign anticommutation relation for the Dirac field?
Consider the Dirac Lagrangian $$\mathcal{L}=\psi ^{\dagger }\gamma ^{0}\left(
\mathrm{i}\gamma ^{\rho }\partial _{\rho }-m\right) \psi .$$ The conjugate
momenta to $\psi ^{a}$ are defined, as usual, …