Two- and Three-Dimensional Electron Traps — Question 7

Section 39-6 · Physics pages 6524–6525

Question 7 Strong confinement in one direction freezes its excitation at low energies In a three-dimensional rectangular infinite well, E = C(n2 x/L2 x + n2 y/L2 y + n2 z/L2 z), with positive integer indices and C = π2ℏ2/(2m). Ignore spin. Let Lx = Ly = L and Lz = L/10. Define A = C/L2. Only excitations at most 20A above the ground energy are accessible. Lx Lz Ly Lz = L/10 Schematic; labels, not drawing lengths, specify the data. (a) Find the ground energy and the lowest excitation gap along each axis. (b) Determine which z mode is accessible and write the effective low-energy two-dimensional spectrum.
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Question 7 - Solution Strong confinement in one direction freezes its excitation at low energies Lx Lz Ly Lz = L/10 (a) Method and calculation E111 = A(1 + 1 + 100) = 102A . ∆Ex = ∆Ey = 3A, ∆Ez = 300A . (b) Interpretation and further calculation 20A < 300A ⇒nz = 1 throughout the accessible subspace . Enxny,1 = 100A + A(n2 x + n2 y) , n2 x + n2 y ≤22. Physical check The frozen direction still contributes a large zero-point energy. Effective two-dimensional motion does not mean that this energy disappears.

Question 7

Strong confinement in one direction freezes its excitation at low energies

In a three-dimensional rectangular infinite well, E=C(nx2/Lx2+ny2/Ly2+nz2/Lz2)E=C(n_x^2/L_x^2+n_y^2/L_y^2+n_z^2/L_z^2), with positive integer indices and C=π2ℏ2/(2m)C=\pi^2\hbar^2/(2m). Ignore spin. Let Lx=Ly=LL_x=L_y=L and Lz=L/10L_z=L/10. Define A=C/L2A=C/L^2. Only excitations at most 20A20A above the ground energy are accessible.

Diagram shown in the original SVG worksheet.

  1. Find the ground energy and the lowest excitation gap along each axis.

  2. Determine which z mode is accessible and write the effective low-energy two-dimensional spectrum.

Question 7 - Solution

Strong confinement in one direction freezes its excitation at low energies

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E111=A(1+1+100)=102A.\boxed{E_{111}=A(1+1+100)=102A}.ΔEx=ΔEy=3A,ΔEz=300A.\boxed{\Delta E_x=\Delta E_y=3A,\qquad\Delta E_z=300A}.

(b) Interpretation and further calculation

20A<300A⇒nz=1 throughout the accessible subspace.20A<300A\Rightarrow\boxed{n_z=1\text{ throughout the accessible subspace}}.Enxny,1=100A+A(nx2+ny2),nx2+ny2≤22.\boxed{E_{n_xn_y,1}=100A+A(n_x^2+n_y^2)},\quad n_x^2+n_y^2\le22.

Physical check

The frozen direction still contributes a large zero-point energy. Effective two-dimensional motion does not mean that this energy disappears.