(a) Show that for any normalized ∣ψ⟩, ⟨ψ∣H∣ψ⟩≥E0, where E0 is the lowest-energy eigenvalue. (Hint: Expand ∣ψ⟩ in the eigenbasis of H.)
(b) Prove the following theorem: Every attractive potential in one dimension has at least one bound state. Hint: Since V is attractive, if we define V(∞)=0, it follows that V(x)=−∣V(x)∣ for all x. To show that there exists a bound state with E<0, consider
ψa(x)=(πa)1/4e−ax2/2
and calculate
E(a)=⟨ψa∣H∣ψa⟩,H=−2mℏ2dx2d2−∣V(x)∣
Show that E(a) can be made negative by a suitable choice of a. The desired result follows from the application of the theorem proved above.