Morrison writes in "Morrison, Michael A. : Understanding quantum physics : a user's manual"
$ |\Psi(x,t)|^2 \xrightarrow[x\rightarrow\pm \infty ]{} 0$ at all times t [bound state]
$ |\Psi(x,t)|^2 \xrightarrow[x\rightarrow\pm \infty ]{} 0$ at any particular time t [unbound state]
So I can imagine that "all" means the entirety of all times, but do I not get "all" when summing over all particular states?
I also understand that in a bound state, the wave is never at the infinity position, but the wave of an unbound state may exist there.
