An electron of mass is confined to an infinite square well of width

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

The Structure of Quantum Mechanics, Ch Hilbert space and Dirac notation

Problem

An electron of mass me=9.109×10−31 kgm_e = 9.109\times10^{-31}\,\mathrm{kg} is confined to an infinite square well of width L=2.00 nmL=2.00\,\mathrm{nm}, with impenetrable walls at x=0x=0 and x=Lx=L. The energy eigenstates ∣n⟩|n\rangle satisfy ⟨x∣n⟩=2/Lsin⁡(nπx/L)\langle x|n\rangle=\sqrt{2/L}\sin(n\pi x/L) and H^∣n⟩=En∣n⟩\hat H|n\rangle=E_n|n\rangle with En=n2π2ℏ2/(2meL2)E_n=n^2\pi^2\hbar^2/(2m_eL^2), where ℏ=1.0546×10−34 J s\hbar = 1.0546\times10^{-34}\,\mathrm{J\,s}. The electron is prepared in the normalised state ∣ψ⟩=15∣1⟩+25∣2⟩.|\psi\rangle=\frac{1}{\sqrt5}|1\rangle+\frac{2}{\sqrt5}|2\rangle. ((a)) Let ∣ψ′⟩=eiπ/4∣ψ⟩|\psi'\rangle=e^{i\pi/4}|\psi\rangle. Compute the probabilities of finding energies E1E_1 and E2E_2 for both ∣ψ⟩|\psi\rangle and ∣ψ′⟩|\psi'\rangle, and compute ⟨H^⟩\langle\hat H\rangle for both. State what this shows about ∣ψ⟩|\psi\rangle and ∣ψ′⟩|\psi'\rangle as physical states. ((b)) Insert the resolution of the identity ∑n∣n⟩⟨n∣=1\sum_n|n\rangle\langle n|=\mathbb 1 into ⟨ψ∣H^∣ψ⟩\langle\psi|\hat H|\psi\rangle to write the energy expectation value as a sum over nn, then evaluate it numerically in electronvolts.

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