More Electron Traps — Question 10

Section 39-5 · Physics pages 6510–6511

Question 10 A sudden increase of trap frequency excites the electron above the new ground state An electron begins in the ground state of a harmonic trap of frequency ω. The frequency suddenly changes to ω′ = 2ω, leaving the wave function unchanged at that instant. Initially ⟨K⟩= ⟨V ⟩= ℏω/4. For two oscillator ground states, use |⟨0ω′|0ω⟩|2 = 2√ωω′/(ω + ω′). x Schematic; labels, not drawing lengths, specify the data. (a) Find the mean energy immediately after the change and its excess over the new ground energy. (b) Find the probability of the new ground state and the total excited-state probability.
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Question 10 - Solution A sudden increase of trap frequency excites the electron above the new ground state x (a) Method and calculation ⟨H′⟩= ⟨K⟩+ 4⟨V ⟩= 5ℏω/4 . E0′ = ℏω′/2 = ℏω ⇒⟨H′⟩−E0′ = ℏω/4 . (b) Interpretation and further calculation P0′ = 2 √ 2 3 = .942809 . Pexcited = 1 −2 √ 2/3 = .0571910 . Physical check The frequency change is sudden, so adiabatic ground-state following does not apply. A high ground-state probability can coexist with a nonzero mean excitation energy.

Question 10

A sudden increase of trap frequency excites the electron above the new ground state

An electron begins in the ground state of a harmonic trap of frequency ω\omega. The frequency suddenly changes to ω′=2ω\omega\prime=2\omega, leaving the wave function unchanged at that instant. Initially ⟨K⟩=⟨V⟩=ℏω/4\langle K\rangle=\langle V\rangle=\hbar\omega/4. For two oscillator ground states, use |⟨0ω′|0ω⟩|2=2ωω′/(ω+ω′)|\langle0_{\omega\prime}|0_\omega\rangle|^2=2\sqrt{\omega\omega\prime}/(\omega+\omega\prime).

Diagram shown in the original SVG worksheet.

  1. Find the mean energy immediately after the change and its excess over the new ground energy.

  2. Find the probability of the new ground state and the total excited-state probability.

Question 10 - Solution

A sudden increase of trap frequency excites the electron above the new ground state

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨H′⟩=⟨K⟩+4⟨V⟩=5ℏω/4.\langle H\prime\rangle=\langle K\rangle+4\langle V\rangle=\boxed{5\hbar\omega/4}.E0′=ℏω′/2=ℏω⇒⟨H′⟩−E0′=ℏω/4.E_0\prime=\hbar\omega\prime/2=\hbar\omega\Rightarrow\boxed{\langle H\prime\rangle-E_0\prime=\hbar\omega/4}.

(b) Interpretation and further calculation

P0′=223=.942809.\boxed{P_0\prime=\frac{2\sqrt2}{3}=.942809}.Pexcited=1−22/3=.0571910.\boxed{P_{\mathrm{excited}}=1-2\sqrt2/3=.0571910}.

Physical check

The frequency change is sudden, so adiabatic ground-state following does not apply. A high ground-state probability can coexist with a nonzero mean excitation energy.