An operator \( \hat{O} \) is linear if:
\[
\hat{O} (a \psi + b \phi) = a \hat{O} \psi + b \hat{O} \phi
\]
where \( a \) and \( b \) are scalars.
- \( x^3 \) is a linear function multiplication operator.
- Parity \( \hat{P} \) is a linear operator since it transforms wavefunctions as \( \psi(x) \to \psi(-x) \).
- \( i\hat{p} \) is the momentum operator, which is linear.
However, time reversal \( \hat{T} \) is an anti-unitary operator, meaning:
\[
\hat{T} (a \psi + b \phi) \neq a \hat{T} \psi + b \hat{T} \phi
\]