An Electron in a Finite Well — Question 2

Section 39-4 · Physics pages 6474–6475

Question 2 The first odd bound state appears only beyond a strict depth-width threshold 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. For an odd state use ψ = A sin kx inside and a decaying exponential outside. x V0 −a a Schematic; labels, not drawing lengths, specify the data. (a) Derive the odd-state eigenvalue condition. (b) Find the threshold for the first odd bound state and explain why equality is excluded.
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Question 2 - Solution The first odd bound state appears only beyond a strict depth-width threshold x V0 −a a (a) Method and calculation A sin ka = B, Ak cos ka = −κB ⇒−k cot ka = κ . −z cot z = √ z2 0 −z2 , π/2 < z < π on the first odd branch. (b) Interpretation and further calculation w →0+ : z →π/2 ⇒z0 > π/2 . z0 = π/2 : κ = 0 ⇒ψoutside = constant ⇒not normalizable . Physical check The threshold state is not a bound state. Every nonzero symmetric attractive well has an even ground state, but it need not have an odd state.

Question 2

The first odd bound state appears only beyond a strict depth-width threshold

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. For an odd state use ψ=Asin⁡kx\psi=A\sin kx inside and a decaying exponential outside.

Diagram shown in the original SVG worksheet.

  1. Derive the odd-state eigenvalue condition.

  2. Find the threshold for the first odd bound state and explain why equality is excluded.

Question 2 - Solution

The first odd bound state appears only beyond a strict depth-width threshold

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Asin⁡ka=B,Akcos⁡ka=−κB⇒−kcot⁡ka=κ.A\sin ka=B,\quad Ak\cos ka=-\kappa B\Rightarrow\boxed{-k\cot ka=\kappa}.−zcot⁡z=z02−z2,π/2<z<πon the first odd branch.\boxed{-z\cot z=\sqrt{z_0^2-z^2}},\qquad\pi/2<z<\pi\ \text{on the first odd branch}.

(b) Interpretation and further calculation

w→0+:z→π/2⇒z0>π/2.w\to0^+:\ z\to\pi/2\Rightarrow\boxed{z_0>\pi/2}.z0=π/2:κ=0⇒ψoutside=constant⇒not normalizable.z_0=\pi/2:\ \kappa=0\Rightarrow\psi_{\mathrm{outside}}=\text{constant}\Rightarrow\boxed{\text{not normalizable}}.

Physical check

The threshold state is not a bound state. Every nonzero symmetric attractive well has an even ground state, but it need not have an odd state.