Energies of a Trapped Electron — Question 10

Section 39-2 · Physics pages 6450–6451

Question 10 Resonant absorption depends on the initial mode as well as photon energy A monochromatic photon has energy 5E1. An infinite well has levels En = n2E1. Consider single-photon absorption with negligible linewidth and recoil. Assume any transition satisfying the stated energy condition is otherwise allowed. n = 1 n = 2 n = 3 E 5E1 Schematic; labels, not drawing lengths, specify the data. (a) Determine whether absorption from the ground mode can reach another bound eigenstate. (b) Repeat for an electron initially in mode 2 and identify the final mode.
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Question 10 - Solution Resonant absorption depends on the initial mode as well as photon energy n = 1 n = 2 n = 3 E 5E1 (a) Method and calculation ni = 1 : n2 fE1 = E1 + 5E1 ⇒n2 f = 6. √ 6 /∈N ⇒no resonant final box eigenstate . (b) Interpretation and further calculation ni = 2 : n2 fE1 = 4E1 + 5E1 = 9E1. nf = 3, E3 −E2 = 5E1 . Physical check Energy conservation is necessary for resonance. Actual transition strengths also depend on coupling matrix elements; those are excluded from this energy-only model.

Question 10

Resonant absorption depends on the initial mode as well as photon energy

A monochromatic photon has energy 5E15E_1. An infinite well has levels En=n2E1E_n=n^2E_1. Consider single-photon absorption with negligible linewidth and recoil. Assume any transition satisfying the stated energy condition is otherwise allowed.

Diagram shown in the original SVG worksheet.

  1. Determine whether absorption from the ground mode can reach another bound eigenstate.

  2. Repeat for an electron initially in mode 2 and identify the final mode.

Question 10 - Solution

Resonant absorption depends on the initial mode as well as photon energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ni=1:nf2E1=E1+5E1⇒nf2=6.n_i=1:\quad n_f^2E_1=E_1+5E_1\Rightarrow n_f^2=6.6∉ℕ⇒no resonant final box eigenstate.\sqrt6\notin\mathbb N\Rightarrow\boxed{\text{no resonant final box eigenstate}}.

(b) Interpretation and further calculation

ni=2:nf2E1=4E1+5E1=9E1.n_i=2:\quad n_f^2E_1=4E_1+5E_1=9E_1.nf=3,E3−E2=5E1.\boxed{n_f=3,\quad E_3-E_2=5E_1}.

Physical check

Energy conservation is necessary for resonance. Actual transition strengths also depend on coupling matrix elements; those are excluded from this energy-only model.