Kittel, Chapter 7, Central Equation

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SUMMARY

The central equation for the Fourier components of waves in a periodic lattice, as stated in Kittel's Chapter 7, is given by the equation (\lambdak-E)*C(k)+\sumUG*C(k-G)=0. The coefficients C(k) are determined by substituting the wavefunction form \psi(x)=\sumC(k)*exp(i(k)x) into the Schrödinger equation, which leads to a system of equations for the coefficients. This method of solving differential equations using Fourier series is a general approach and not limited to solid-state physics or Bloch functions.

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Homework Statement


Kittel states at page 172, that the central equation for the Fourier components of waves in a periodic lattice is given by:
([tex]\lambda[/tex]k-E)*C(k)+[tex]\sum[/tex]UG*C(k-G)=0

From this he goes on to say "Once we determine the C's from (27), the wavefunctions (25) is given as:

[tex]\psi[/tex]k(x)=[tex]\sum[/tex]C(k-G)*exp(i(k-G)x)

I'm completely in the blank about how he got the C's isolated and got the above equation for the wavefunction..any help?

Homework Equations



Equation 27:
([tex]\lambda[/tex]k-E)*C(k)+[tex]\sum[/tex]UG*C(k-G)=0

Equation 25:
[tex]\psi[/tex](x)=[tex]\sum[/tex]C(k)*exp(i(k)x)
 
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He did not actually get the coefficients.
He even tells you that solving the equation is a very difficult task in general.
He tells what can be done after the equation is solved.

About how he gets the wave-function: he assumes that it can be written in the form (25), as a combination of plane waves, with various coefficient. (This form is like a Fourier expansion)
To find the coefficients, you plug in the function in Schrödinger eq (the one with Bloch functions) and you get some equations for the coefficients.

This is actually a quite general method of solving differential equations, by using Fourier series. Is not something specific for solid state or Bloch functions.
 

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