How to Evaluate Integrals in Tight Binding Model?

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SUMMARY

The discussion focuses on evaluating integrals within the context of the tight-binding model in solid-state physics. The energy of an electron is expressed using the formula E(k) = -α - γΣ_{m} exp(-ikρ_{m}), where α and γ are integrals that need to be determined. The wavefunction φ(x) is defined piecewise, and the evaluation of the integral γ requires careful consideration of the cases 2x_{0} ≤ ρ and 2x_{0} > ρ. The user seeks clarification on the definitions of φ_{m} and φ_{n}, as well as the significance of the variable ρ in relation to x_{0}.

PREREQUISITES
  • Understanding of the tight-binding model in solid-state physics
  • Familiarity with quantum mechanics, particularly eigenstates and Hamiltonians
  • Knowledge of integral calculus and its application in physics
  • Basic concepts of wavefunctions and their properties
NEXT STEPS
  • Study the derivation of the tight-binding model and its applications in solid-state physics
  • Learn about the evaluation of integrals in quantum mechanics, specifically in the context of wavefunctions
  • Research the significance of the Hamiltonian operator in determining energy levels
  • Explore graphical representations of energy bands in one-dimensional systems
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Students and researchers in physics, particularly those focusing on solid-state physics and quantum mechanics, as well as anyone involved in computational modeling of electronic properties in materials.

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Homework Statement



The energy of an electron within a band as a function of its wavevector is given by the
tight-binding expression (in one dimension),

E(k)=-[itex]\alpha[/itex]-[itex]\gamma[/itex][itex]\Sigma[/itex][itex]_{m}[/itex] exp (-ik[itex]\rho[/itex][itex]_{m}[/itex])

(a)What are typical expressions for integrals [itex]\alpha[/itex] and [itex]\gamma[/itex]?
(b) Evaluate the integral [itex]\gamma[/itex] for the following wavefunction, assuming it is an eigenstate of the Hamiltonian, being careful to distinguish the cases 2x[itex]_{0}[/itex][itex]\leq[/itex][itex]\rho[/itex] and 2x[itex]_{0}[/itex]>[itex]\rho[/itex]:

[itex]\phi[/itex](x)=[itex]\sqrt{\frac{1}{2x_{0}}}[/itex] |x|[itex]\leq[/itex]x[itex]_{0}[/itex]

[itex]\phi[/itex](x)=0 |x|>x[itex]_{0}[/itex]

(c) Hence evaluate the energy of an electron in a linear chain of these atoms with a
spacing a and make a graph of the result for the two cases 2x0 a and 2x0 > a.

The Attempt at a Solution



[itex]\alpha[/itex]=-<[itex]\phi[/itex][itex]_{n}[/itex]|H|[itex]\phi[/itex][itex]_{n}[/itex]>
[itex]\gamma[/itex]=-<[itex]\phi[/itex][itex]_{m}[/itex]|H|[itex]\phi[/itex][itex]_{n}[/itex]>

But I cannot do part b) because I do not know what [itex]\phi[/itex][itex]_{m}[/itex] and [itex]\phi[/itex][itex]_{n}[/itex] are. All that I know is that sometimes n=m and sometimes it does not. Please help.
 
Physics news on Phys.org
What is [itex]\rho[/itex]? Why does it matter whether [itex]\rho[/itex] is bigger or smaller than x[itex]_{0}[/itex]?
 

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