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It is known that in Lorentz-violating effective field theory, there is aclassical equivalence between certain coefficients ($c$ and $f$), in spite ofthe fact that the operators the two types of coefficients describe appear tohave opposite behaviors under $\textbf{CPT}$. This paper is a continuation ofprevious work extending this equivalence to the quantum level: generalizing theexplicit spinorial point transformations that interconvert the $c$ and $f$terms; demonstrating that the transformations do not give rise to anyadditional anomaly terms as the quantum level; and giving explicitprescriptions for modifying the $\textbf{C}$, $\textbf{P}$, and $\textbf{T}$operators in the $f$ theory, so that they correspond to the correctinterchanges of physical particle states.

Aspects of the Equivalence Between the $f^{\mu}$ and $c^{\nu\mu}$ Terms in Lorentz-Violating Quantum Field Theory