Chapter 6 showed that a taller rectangular barrier (larger

PHYSICS · Subjective · Fermi University Physics · Quantum Mechanics · Symmetry, angular momentum and spin · Symmetry, angular momentum and spin

Quantum Mechanics: From the Photon to the Hydrogen Atom, Ch Spin one-half, the Pauli matrices and two-level systems

Problem

Chapter 6 showed that a taller rectangular barrier (larger V0−EV_0-E, hence larger κ=2m(V0−E)/ℏ\kappa = \sqrt{2m(V_0-E)}/\hbar) suppresses tunnelling transmission exponentially, T≈16E(V0−E)V0−2e−2κa\mathcal T \approx 16E(V_0-E)V_0^{-2}e^{-2\kappa a}. The nitrogen crossing ammonia's barrier is exactly this kind of tunnelling, though Δ\Delta is fixed by the measured line rather than computed from the barrier. Suppose a related molecule had a taller barrier between its two configurations than ammonia's, with everything else the same. Without computing a new value for Δ\Delta, say whether this molecule's inversion line would sit above or below ammonia's 23.9 GHz23.9\ \mathrm{GHz}, and whether its crossing time would be longer or shorter than ammonia's 2.1×10−11 s2.1\times10^{-11}\ \mathrm s, giving the chain of reasoning that connects the two chapters.

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