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