Energies of a Trapped Electron — Question 4

Section 39-2 · Physics pages 6438–6439

Question 4 An energy cutoffpermits only a finite number of box modes An electron in an infinite well is prepared using only eigenstates with En ≤Ecut = 10E1. Spin is not included. The energy levels are En = n2E1. n = 1 n = 2 n = 3 E Ecut Schematic; labels, not drawing lengths, specify the data. (a) List the permitted mode indices and count them. (b) Generalize the count to arbitrary positive Ecut and evaluate it just below 9E1.
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Question 4 - Solution An energy cutoffpermits only a finite number of box modes n = 1 n = 2 n = 3 E Ecut (a) Method and calculation n2 ≤10 ⇒n ≤ √ 10 ⇒n = 1, 2, 3 . N = 3 spatial eigenstates. (b) Interpretation and further calculation N(Ecut) = ⌊√ Ecut/E1 ⌋ . Ecut = 9E1 −ϵ, 0 < ϵ ≪E1 ⇒N = 2 . Physical check The count is a staircase, not a continuous density of states. The distinction between below and at a threshold matters for the highest permitted mode.

Question 4

An energy cutoff permits only a finite number of box modes

An electron in an infinite well is prepared using only eigenstates with En≤Ecut=10E1E_n\le E_{\mathrm{cut}}=10E_1. Spin is not included. The energy levels are En=n2E1E_n=n^2E_1.

Diagram shown in the original SVG worksheet.

  1. List the permitted mode indices and count them.

  2. Generalize the count to arbitrary positive EcutE_{\mathrm{cut}} and evaluate it just below 9E19E_1.

Question 4 - Solution

An energy cutoff permits only a finite number of box modes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n2≤10⇒n≤10⇒n=1,2,3.n^2\le10\Rightarrow n\le\sqrt{10}\Rightarrow\boxed{n=1,2,3}.N=3spatial eigenstates.\boxed{N=3}\quad\text{spatial eigenstates}.

(b) Interpretation and further calculation

N(Ecut)=⌊Ecut/E1⌋.\boxed{N(E_{\mathrm{cut}})=\left\lfloor\sqrt{E_{\mathrm{cut}}/E_1}\right\rfloor}.Ecut=9E1−ϵ,0<ϵ≪E1⇒N=2.E_{\mathrm{cut}}=9E_1-\epsilon,\quad0<\epsilon\ll E_1\Rightarrow\boxed{N=2}.

Physical check

The count is a staircase, not a continuous density of states. The distinction between below and at a threshold matters for the highest permitted mode.