An Electron in a Finite Well — Question 8

Section 39-4 · Physics pages 6486–6487

Question 8 Deep-well leakage can be approximated as an increase of effective width A deep finite well has physical width L and a nearly constant exterior decay constant κ. Use the approximation Leff= L + 2/κ and En ≃n2π2ℏ2/(2mL2 eff). The corresponding infinite-well energy is E(∞) n = n2π2ℏ2/(2mL2). x V0 −a a Schematic; labels, not drawing lengths, specify the data. (a) Derive the energy ratio and its first correction for κL ≫1. (b) Evaluate the effective-width ratio and its linear approximation at κL = 20.
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Question 8 - Solution Deep-well leakage can be approximated as an increase of effective width x V0 −a a (a) Method and calculation En E(∞) n ≃ ( 1 + 2 κL )−2 . En/E(∞) n ≃1 −4 κL + O((κL)−2) . (b) Interpretation and further calculation κL = 20 : (1 + .1)−2 = .826446 . 1 −4/20 = .800000 . Physical check The numerical ratio is exact only within the effective-width approximation. A true finite-well calculation must account for the energy dependence of the decay constant.

Question 8

Deep-well leakage can be approximated as an increase of effective width

A deep finite well has physical width L and a nearly constant exterior decay constant κ\kappa. Use the approximation Leff=L+2/κL_{\mathrm{eff}}=L+2/\kappa and En≃n2π2ℏ2/(2mLeff2)E_n\simeq n^2\pi^2\hbar^2/(2mL_{\mathrm{eff}}^2). The corresponding infinite-well energy is En(∞)=n2π2ℏ2/(2mL2)E_n^{(\infty)}=n^2\pi^2\hbar^2/(2mL^2).

Diagram shown in the original SVG worksheet.

  1. Derive the energy ratio and its first correction for κL≫1\kappa L\gg1.

  2. Evaluate the effective-width ratio and its linear approximation at κL=20\kappa L=20.

Question 8 - Solution

Deep-well leakage can be approximated as an increase of effective width

Diagram shown in the original SVG worksheet.

(a) Method and calculation

EnEn(∞)≃(1+2κL)−2.\boxed{\frac{E_n}{E_n^{(\infty)}}\simeq\left(1+\frac2{\kappa L}\right)^{-2}}.En/En(∞)≃1−4κL+O((κL)−2).\boxed{E_n/E_n^{(\infty)}\simeq1-\frac4{\kappa L}+O((\kappa L)^{-2})}.

(b) Interpretation and further calculation

κL=20:(1+.1)−2=.826446.\kappa L=20:\quad\boxed{(1+.1)^{-2}=.826446}.1−4/20=.800000.\boxed{1-4/20=.800000}.

Physical check

The numerical ratio is exact only within the effective-width approximation. A true finite-well calculation must account for the energy dependence of the decay constant.