Principles of Quantum Mechanics · Problem 5.2.2

Simple Problems in One Dimension — R. Shankar

Physics — Quantum Mechanics · attractive-potential-bound-state

Problem

(a) Show that for any normalized ∣ψ⟩|\psi\rangle, ⟨ψ∣H∣ψ⟩≥E0\langle \psi|H|\psi\rangle \geq E_0, where E0E_0 is the lowest-energy eigenvalue. (Hint: Expand ∣ψ⟩|\psi\rangle in the eigenbasis of HH.) (b) Prove the following theorem: Every attractive potential in one dimension has at least one bound state. Hint: Since VV is attractive, if we define V(∞)=0V(\infty) = 0, it follows that V(x)=−∣V(x)∣V(x) = -|V(x)| for all xx. To show that there exists a bound state with E<0E < 0, consider ψa(x)=(aπ)1/4e−ax2/2\psi_a(x) = \left(\frac{a}{\pi}\right)^{1/4} e^{-ax^2/2} and calculate E(a)=⟨ψa∣H∣ψa⟩,H=−ℏ22md2dx2−∣V(x)∣E(a) = \langle \psi_a | H | \psi_a \rangle, \quad H = -\frac{\hbar^2}{2m}\frac{d^2}{dx^2} - |V(x)| Show that E(a)E(a) can be made negative by a suitable choice of aa. The desired result follows from the application of the theorem proved above.

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