Dynamics of electron in crystal lattice

  • Thread starter paweld
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  • #1
paweld
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I'm not sure what is the correct equation for motion of electron in a crystal
lattice under the influence of magnetic force. On may easily proof that for
electric force the following equation holds (the proof might be found in
http://ajp.aapt.org/resource/1/ajpias/v54/i2/p177_s1" [Broken] ):
[tex]
\hbar \frac{d}{d t} \langle T \rangle = -e E
[/tex]
(T - lattice translation opertor; its eigenvalues are called usually quasimomentum;
here we have average value). Straightforward modification of above equation
which incorporate magnetic force would be (E(k) means energy):
[tex]
\hbar \frac{d}{d t} \langle T \rangle = -e (\vec{E} + \frac{1}{\hbar}\nabla_{\vec{k}}E(k)\times \vec{B})
[/tex]
And this equation is stated by most textbooks concering solid state physics (however
without proof or with proof which is not rigorous). Does anyone know a good proof
of these equation?
 
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Answers and Replies

  • #2
kanato
415
1
If you look in appendix E of Ashcroft and Mermin, there is a rigorous proof that the expectation value of the velocity operator is [tex] \nabla_k E(k)[/tex]. Since the equation you wrote is basically the Lorentz force equation, I suspect you could derive it from that and Ehrenfest's theorem.
 
  • #3
paweld
255
0
Using Ehrenfest theorem one would obtain the following formula
[tex]
\hbar \frac{d}{d t} \langle p\rangle = -e (\vec{E} + \frac{1}{\hbar}\nabla_{\vec{k}}E(k)\times \vec{B})
[/tex]
where p is momentum of electron and it is different from quasimomentum
which is usually denoted by k. Most textbooks gives this formula with k
not p and this is why I'm wondering why it's true.
 
Last edited:
  • #4
DrDu
Science Advisor
6,256
906
Ashcroft and Mermin discuss this topic quite at length and, more importantly, give many links to relevant literature.
 

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