 Solution

On Bob's polarization qubit, takeSuitable conditional unitary operators areIndeed $(I\otimes XZ)|{\Phi }^{+}⟩=|{\Psi }^{-}⟩$, $(I\otimes X)|{\Phi }^{-}⟩=|{\Psi }^{-}⟩$, and $(I\otimes Z)|{\Psi }^{+}⟩=-|{\Psi }^{-}⟩$. The last minus sign is a harmless global phase.

For an ideal half-wave plate whose fast axis makes angle $\theta$ with horizontal polarization, discard the common phase and use the Jones matrixIt implements $Z$ at $0^{\circ }$ and $X$ at $45^{\circ }$. Thus for outcome ${\Phi }^{+}$ use two half-wave plates, first $0^{\circ }$ then $45^{\circ }$ in the propagation direction; for ${\Phi }^{-}$ use one at $45^{\circ }$; for ${\Psi }^{+}$ one at $0^{\circ }$; for ${\Psi }^{-}$ use no plate. Ideal retardance is assumed at the photon wavelength, and the setting is chosen after receiving the detector's classical result.