An Electron in a Finite Well — Question 9

Section 39-4 · Physics pages 6488–6489

Question 9 Sensitivity to wall height directly measures exterior probability A symmetric finite well has V = 0 for |x| < a and V = V0 > 0 outside. Bound energies satisfy 0 < E < V0. Define k = √ 2mE/ℏ, κ = √ 2m(V0 −E)/ℏ, z = ka, w = κa and z0 = a√2mV0/ℏ. Use the Hellmann–Feynman relation dE/dV0 = ⟨∂H/∂V0⟩for a normalized nondegenerate bound state at fixed a. The potential is zero inside and V0 outside. x V0 −a a δV0 Schematic; labels, not drawing lengths, specify the data. (a) Relate the energy slope to the probability outside. (b) If dE/dV0 = .180, find the slope of the binding energy B = V0 −E and both spatial probabilities.
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Question 9 - Solution Sensitivity to wall height directly measures exterior probability x V0 −a a δV0 (a) Method and calculation ∂H/∂V0 = 0 (|x| < a), 1 (|x| > a). dE/dV0 = ∫ |x|>a |ψ|2dx = Pout . (b) Interpretation and further calculation Pout = .180, Pin = .820 . dB/dV0 = 1 −dE/dV0 = Pin = .820 . Physical check Both slopes lie between zero and one. This derivative holds at fixed width and mass, with the energy zero fixed at the well bottom.

Question 9

Sensitivity to wall height directly measures exterior probability

A symmetric finite well has V=0V=0 for |x|<a|x|<a and V=V0>0V=V_0>0 outside. Bound energies satisfy 0<E<V00<E<V_0. Define k=2mE/ℏk=\sqrt{2mE}/\hbar, κ=2m(V0−E)/ℏ\kappa=\sqrt{2m(V_0-E)}/\hbar, z=kaz=ka, w=κaw=\kappa a and z0=a2mV0/ℏz_0=a\sqrt{2mV_0}/\hbar. Use the Hellmann–Feynman relation dE/dV0=⟨∂H/∂V0⟩dE/dV_0=\langle\partial H/\partial V_0\rangle for a normalized nondegenerate bound state at fixed a. The potential is zero inside and V0V_0 outside.

Diagram shown in the original SVG worksheet.

  1. Relate the energy slope to the probability outside.

  2. If dE/dV0=.180dE/dV_0=.180, find the slope of the binding energy B=V0−EB=V_0-E and both spatial probabilities.

Question 9 - Solution

Sensitivity to wall height directly measures exterior probability

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂H/∂V0=0(|x|<a),1(|x|>a).\partial H/\partial V_0=0\ (|x|<a),\quad1\ (|x|>a).dE/dV0=∫|x|>a|ψ|2dx=Pout.\boxed{dE/dV_0=\int_{|x|>a}|\psi|^2dx=P_{\mathrm{out}}}.

(b) Interpretation and further calculation

Pout=.180,Pin=.820.\boxed{P_{\mathrm{out}}=.180,\qquad P_{\mathrm{in}}=.820}.dB/dV0=1−dE/dV0=Pin=.820.\boxed{dB/dV_0=1-dE/dV_0=P_{\mathrm{in}}=.820}.

Physical check

Both slopes lie between zero and one. This derivative holds at fixed width and mass, with the energy zero fixed at the well bottom.