A particle of mass is constrained to move on a rigid circular ring of radius
PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · The formalism of quantum mechanics · The formalism of quantum mechanics
The Structure of Quantum Mechanics, Ch Position, momentum and the origin of the canonical commutator
Problem
A particle of mass m is constrained to move on a rigid circular ring of radius R, with position measured by arc length s around the ring, s∈[0,L) where L=2πR is the circumference. Translation by an arc length a along the ring is generated by the momentum exactly as on an infinite line, T^(a)=e−iap^/ℏ, and the free-particle Hamiltonian (no potential acts on the ring) is H^=p^2/2m.Because the ring closes on itself, translating all the way around it must return every state to itself up to at most an overall phase: T^(L)∣ψ⟩=eiα∣ψ⟩ for every state ∣ψ⟩, where α is a fixed real number, the same for every state (a property of the ring, not of the particular state).
((a)) Working in the momentum representation, use T^(L)∣p⟩=e−iLp/ℏ∣p⟩ together with the boundary condition above to show that the allowed momentum eigenvalues form the discrete set pn=Rℏ(n−2πα),n=0,±1,±2,…
((b)) Take the periodic case α=0. Write down the energy eigenvalues En and identify the two lowest distinct energies.
((c)) State, with a one-line reason, whether the position or the momentum representation makes finding this spectrum easier, given that [H^,p^]=0 for a free particle on the line or on the ring.
((d)) An electron of mass m=9.109×10−31kg is confined to such a ring with R=2.0nm and α=0. Compute, in electronvolts, the energy of the first excited level above the ground state.