An oscillator has mass and angular frequency

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Wave mechanics in one dimension · The formalism of quantum mechanics

The Structure of Quantum Mechanics, Ch The oscillator as an algebra

Problem

An oscillator has mass m=2.0×10−26 kgm = 2.0\times10^{-26}\ \mathrm{kg} and angular frequency ω=5.0×1013 rad s−1\omega = 5.0\times10^{13}\ \mathrm{rad\,s^{-1}}, and is in the number state ∣n⟩|n\rangle with n=3n=3. ((a)) Using the counting results ⟨n∣x^∣n⟩=⟨n∣p^∣n⟩=0\langle n|\hat x|n\rangle = \langle n|\hat p|n\rangle = 0 (from the selection rule that x^\hat x and p^\hat p connect ∣n⟩|n\rangle only to ∣n±1⟩|n\pm1\rangle) and ⟨n∣x^2∣n⟩=(n+12)ℏ/mω\langle n|\hat x^2|n\rangle = (n+\tfrac12)\hbar/m\omega, ⟨n∣p^2∣n⟩=(n+12)mℏω\langle n|\hat p^2|n\rangle = (n+\tfrac12)m\hbar\omega, compute Δx\Delta x and Δp\Delta p numerically for ∣3⟩|3\rangle. ((b)) Compute the product Δx Δp\Delta x\,\Delta p and compare it with the generalised uncertainty relation Δx Δp≥ℏ/2\Delta x\,\Delta p \ge \hbar/2. State for which nn equality holds, and connect that state to the Gaussian ground-state wave function produced from the lowering condition a^∣0⟩=0\hat a|0\rangle=0.

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