2D problem of nearly free electron model

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SUMMARY

The discussion focuses on solving a 2D problem within the nearly free electron model, specifically finding the energies of states at the point \((\frac{\pi}{a},0)\) and deriving the secular equation. The energy equation is established as \(E = \epsilon_0 \pm \sqrt{V_{10}^2 + V_{11}^2}\), where \(V(x,y)\) is expressed in complex notation involving terms \(V_{10}\) and \(V_{11}\). The central equation for the secular problem is given by \((\epsilon_0 - E) C_{(k)} + \sum\limits_{G} U_G ~ C_{(k-G)} = 0\), which leads to the need for constructing a 4x4 matrix for further analysis.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the nearly free electron model.
  • Familiarity with complex notation in physics.
  • Knowledge of matrix algebra, specifically in the context of eigenvalue problems.
  • Experience with Fourier series and their application in potential energy calculations.
NEXT STEPS
  • Study the derivation of the secular equation in the context of solid-state physics.
  • Learn about constructing and solving eigenvalue problems using 4x4 matrices.
  • Explore the implications of the nearly free electron model on band structure in solids.
  • Investigate the role of potential energy terms \(V_{10}\) and \(V_{11}\) in determining electronic states.
USEFUL FOR

Students and researchers in condensed matter physics, particularly those focusing on electronic properties of materials and band theory. This discussion is also beneficial for anyone studying quantum mechanics and solid-state physics.

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Homework Statement



(a) Find energies of states at ##(\frac{\pi}{a},0)##.
(b) Find secular equation

simon_15_4.png

Homework Equations

The Attempt at a Solution



Part(a)[/B]
In 1D, the secular equation for energy is:
E = \epsilon_0 \pm \left| V(x,y) \right|

When represented in complex notation, the potential becomes
V(x,y) = V_{10} \left[ e^{i\frac{2\pi x}{a}} + e^{-i\frac{2\pi x}{a}} + e^{i\frac{2\pi y}{a}} + e^{-i\frac{2\pi y}{a}} \right] + V_{11} \left[ e^{i\frac{2\pi x}{a}} + e^{-i\frac{2\pi x}{a}} \right] \left[ e^{i\frac{2\pi y}{a}} + e^{-i\frac{2\pi y}{a}} \right]

E = \epsilon_0 \pm \sqrt{V_{10}^2 + V_{11}^2 }

Part(b)
I know the central equation is given by
\left(\epsilon_0 - E \right) C_{(k)} + \sum\limits_{G} U_G ~ C_{(k-G)} = 0

How do I find the 4x4 matrix?
 
bumpp
 
bumpp
 

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