Energies of a Trapped Electron — Question 5

Section 39-2 · Physics pages 6440–6441

Question 5 A mean energy need not equal an allowed measurement outcome An electron is in the normalized state √ 3/4 u1 + eiα√ 1/4 u3, where the orthonormal box eigenstates have energies En = n2E1. n = 1 n = 3 E P = 3/4 P = 1/4 Schematic; labels, not drawing lengths, specify the data. (a) Find the probabilities of each energy outcome and the mean energy. (b) Find the energy standard deviation and determine whether changing α changes these statistics.
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Question 5 - Solution A mean energy need not equal an allowed measurement outcome n = 1 n = 3 E P = 3/4 P = 1/4 (a) Method and calculation P(E1) = 3/4, P(9E1) = 1/4 . ⟨E⟩= (3/4)E1 + (1/4)9E1 = 3E1 . (b) Interpretation and further calculation ⟨E2⟩= (3/4)E2 1 + (1/4)81E2 1 = 21E2 1. σE = √ 21 −9 E1 = 2 √ 3 E1 , ∂α⟨E⟩= ∂ασE = 0 . Physical check The mean is an ensemble statistic and need not be an eigenvalue. Relative phase can affect other observables even though it cancels from these energy probabilities.

Question 5

A mean energy need not equal an allowed measurement outcome

An electron is in the normalized state 3/4u1+eiα1/4u3\sqrt{3/4}\,u_1+e^{i\alpha}\sqrt{1/4}\,u_3, where the orthonormal box eigenstates have energies En=n2E1E_n=n^2E_1.

Diagram shown in the original SVG worksheet.

  1. Find the probabilities of each energy outcome and the mean energy.

  2. Find the energy standard deviation and determine whether changing α\alpha changes these statistics.

Question 5 - Solution

A mean energy need not equal an allowed measurement outcome

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P(E1)=3/4,P(9E1)=1/4.\boxed{P(E_1)=3/4,\quad P(9E_1)=1/4}.⟨E⟩=(3/4)E1+(1/4)9E1=3E1.\boxed{\langle E\rangle=(3/4)E_1+(1/4)9E_1=3E_1}.

(b) Interpretation and further calculation

⟨E2⟩=(3/4)E12+(1/4)81E12=21E12.\langle E^2\rangle=(3/4)E_1^2+(1/4)81E_1^2=21E_1^2.σE=21−9E1=23E1,∂α⟨E⟩=∂ασE=0.\boxed{\sigma_E=\sqrt{21-9}\,E_1=2\sqrt3\,E_1},\quad\boxed{\partial_\alpha\langle E\rangle=\partial_\alpha\sigma_E=0}.

Physical check

The mean is an ensemble statistic and need not be an eigenvalue. Relative phase can affect other observables even though it cancels from these energy probabilities.