Introduction to Quantum Mechanics · Problem 2.45

Time-Independent Schrödinger Equation — David J. Griffiths

Physics — Quantum Mechanics · node_theorem

Problem

In this problem you will show that the number of nodes of the stationary states of a one-dimensional potential always increases with energy. Consider two (real, normalized) solutions (ψn\psi_n and ψm\psi_m) to the time-independent Schrödinger equation (for a given potential V(x)V(x)), with energies En>EmE_n > E_m. (a) Show that ddx(dψmdxψn−ψmdψndx)=2mℏ2(En−Em)ψmψn.\frac{d}{dx}\left(\frac{d\psi_m}{dx}\psi_n - \psi_m\frac{d\psi_n}{dx}\right) = \frac{2m}{\hbar^2}(E_n - E_m)\psi_m\psi_n. (b) Let x1x_1 and x2x_2 be two adjacent nodes of the function ψm(x)\psi_m(x). Show that ψm′(x2)ψn(x2)−ψm′(x1)ψn(x1)=2mℏ2(En−Em)∫x1x2ψmψn dx.\psi_m'(x_2)\psi_n(x_2) - \psi_m'(x_1)\psi_n(x_1) = \frac{2m}{\hbar^2}(E_n - E_m)\int_{x_1}^{x_2}\psi_m\psi_n\,dx. (c) If ψn(x)\psi_n(x) has no nodes between x1x_1 and x2x_2, then it must have the same sign everywhere in the interval. Show that (b) then leads to a contradiction. Therefore, between every pair of nodes of ψm(x)\psi_m(x), ψn(x)\psi_n(x) must have at least one node, and in particular the number of nodes increases with energy.

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