Energy Levels in a Crystalline Solid — Question 10

Section 41-2 · Physics pages 6830–6831

Question 10 An avoided crossing exchanges orbital character while maintaining a finite gap Two crystal orbitals have bare energies E0 + δ and E0 −δ, coupled by real t. Use H = ( E0 + δ t t E0 −δ ) . δ Schematic; labels, not drawing lengths, specify the data. (a) Derive the eigenenergies and minimum separation as δ varies. (b) For δ = 3t and t > 0, find the splitting and compare it with the uncoupled separation.
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Question 10 - Solution An avoided crossing exchanges orbital character while maintaining a finite gap δ (a) Method and calculation det(H −EI) = (E0 −E)2 −δ2 −t2 = 0. E± = E0 ± √ δ2 + t2, ∆Emin = 2|t| . (b) Interpretation and further calculation δ = 3t : ∆E = 2 √ 10 t = 6.325t . ∆Et=0 = 2|δ| = 6t ⇒∆E/(2|δ|) = √ 10/3 = 1.054 . Physical check The minimum gap is nonzero for nonzero coupling. Far from the crossing, eigenstates approach their bare-orbital character; near the crossing they mix strongly.

Question 10

An avoided crossing exchanges orbital character while maintaining a finite gap

Two crystal orbitals have bare energies E0+δE_0+\delta and E0−δE_0-\delta, coupled by real t. Use H=(E0+δttE0−δ)H=\begin{pmatrix}E_0+\delta&t\\t&E_0-\delta\end{pmatrix}.

Diagram shown in the original SVG worksheet.

  1. Derive the eigenenergies and minimum separation as δ\delta varies.

  2. For δ=3t\delta=3t and t>0t>0, find the splitting and compare it with the uncoupled separation.

Question 10 - Solution

An avoided crossing exchanges orbital character while maintaining a finite gap

Diagram shown in the original SVG worksheet.

(a) Method and calculation

det⁡(H−EI)=(E0−E)2−δ2−t2=0.\det(H-EI)=(E_0-E)^2-\delta^2-t^2=0.E±=E0±δ2+t2,ΔEmin=2|t|.\boxed{E_\pm=E_0\pm\sqrt{\delta^2+t^2},\quad\Delta E_{\min}=2|t|}.

(b) Interpretation and further calculation

δ=3t:ΔE=210t=6.325t.\delta=3t:\quad\boxed{\Delta E=2\sqrt{10}\,t=6.325t}.ΔEt=0=2|δ|=6t⇒ΔE/(2|δ|)=10/3=1.054.\Delta E_{t=0}=2|\delta|=6t\Rightarrow\boxed{\Delta E/(2|\delta|)=\sqrt{10}/3=1.054}.

Physical check

The minimum gap is nonzero for nonzero coupling. Far from the crossing, eigenstates approach their bare-orbital character; near the crossing they mix strongly.