Two- and Three-Dimensional Electron Traps — Question 2

Section 39-6 · Physics pages 6514–6515

Question 2 Square-well degeneracy depends on sums of squares rather than a single index In a rectangular infinite well, Enxny = C(n2 x/L2 x + n2 y/L2 y), where C = π2ℏ2/(2m) and each index is a positive integer. Ignore spin. Let Lx = Ly = L and A = C/L2. x y Lx Ly Schematic; labels, not drawing lengths, specify the data. (a) List all states at energies 5A and 8A. (b) List all states at 10A and give the spatial degeneracy of each energy.
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Question 2 - Solution Square-well degeneracy depends on sums of squares rather than a single index x y Lx Ly (a) Method and calculation n2 x + n2 y = 5 ⇒(1, 2), (2, 1) . n2 x + n2 y = 8 ⇒(2, 2) . (b) Interpretation and further calculation n2 x + n2 y = 10 ⇒(1, 3), (3, 1) . g(5A) = 2, g(8A) = 1, g(10A) = 2 . Physical check Interchanging unequal indices produces distinct states at equal energy in a square. Equal indices produce only one state, and zero indices are excluded.

Question 2

Square-well degeneracy depends on sums of squares rather than a single index

In a rectangular infinite well, Enxny=C(nx2/Lx2+ny2/Ly2)E_{n_xn_y}=C(n_x^2/L_x^2+n_y^2/L_y^2), where C=π2ℏ2/(2m)C=\pi^2\hbar^2/(2m) and each index is a positive integer. Ignore spin. Let Lx=Ly=LL_x=L_y=L and A=C/L2A=C/L^2.

Diagram shown in the original SVG worksheet.

  1. List all states at energies 5A5A and 8A8A.

  2. List all states at 10A10A and give the spatial degeneracy of each energy.

Question 2 - Solution

Square-well degeneracy depends on sums of squares rather than a single index

Diagram shown in the original SVG worksheet.

(a) Method and calculation

nx2+ny2=5⇒(1,2),(2,1).n_x^2+n_y^2=5\Rightarrow\boxed{(1,2),(2,1)}.nx2+ny2=8⇒(2,2).n_x^2+n_y^2=8\Rightarrow\boxed{(2,2)}.

(b) Interpretation and further calculation

nx2+ny2=10⇒(1,3),(3,1).n_x^2+n_y^2=10\Rightarrow\boxed{(1,3),(3,1)}.g(5A)=2,g(8A)=1,g(10A)=2.\boxed{g(5A)=2,\quad g(8A)=1,\quad g(10A)=2}.

Physical check

Interchanging unequal indices produces distinct states at equal energy in a square. Equal indices produce only one state, and zero indices are excluded.