I am reading book called "A Unified Grand Tour of Theoretical Physics" by Ian D Lawrie. I have started bra ket notation and state vectors. Could somebody explain to me how $$P(a,b,c..| \Psi) = |\langle a,b,c...|\Psi\rangle| ^2.$$
$a,b,c$ are called observable quantities. $\Psi$ has been normalised. I come from a background of using wavefunctions and not state vectors and Dirac notation. For me a probability comes from $\Psi \Psi^*$ or $\Psi \Psi$. Perhaps I haven't understood what a state vector is.