Teleportation with the psi-plus Bell state
= Teleportation with the psi-plus Bell state
When the shared resource is $|\Psi^+\rangle$, Bell outcomes $\Phi^+,\Phi^-,\Psi^+,\Psi^-$ leave the receiver with $X|\alpha\rangle,XZ|\alpha\rangle,|\alpha\rangle,Z|\alpha\rangle$, respectively, up to global phases.