I understanding the meaning of Bloch waves

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SUMMARY

This discussion centers on the interpretation of Bloch waves in the context of electron behavior in periodic potentials. The user explores the implications of the wave function notation α|k> + β|k'>, questioning whether it represents a superposition of scattered and non-scattered states. The responses clarify that while k and k-G represent different wave functions with distinct frequencies and energies, they belong to the same irreducible representation of translation symmetry, leading to energy gaps in semiconductors due to mixing at Brillouin zone edges.

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  • Familiarity with periodic potentials and their mathematical representation
  • Knowledge of wave functions and superposition in quantum mechanics
  • Concept of Brillouin zones in solid-state physics
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Before reading Bloch theorem i read something to get a feeling to what happens to the energy of electron in a periodic potential, in short what i read said:
Assuming we have a weak periodic potential from -π/a to π/a for example cos(2πx/a), we can write the electron wave function as: α|k>+β|k'>.
my first question is: does this notation mean that the electron is in superposition state of two states, first one being the electron didn't scatter and the second being the electron did scatter?
After that i went on to read Bloch theorem, he stated that the waving function can be written as:
Σukeikr. and using Fourier series
Σαk-Gei(k-G)r.
my second question is: correct if I'm wrong but since there is no difference between k and k-G in term of energy does that mean that they are the same state? what does the wave function exactly tell us about the electron? for example what does
αk-G1ei(k-G1)rk-G2ei(k-G2)r mean?
sorry for the long question I'm just have a hard time trying to connect the dots
 
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''Since there is no difference between k and k-G in term of energy does that mean that they are the same state?''

In general a point k and the point k-G (or k+G or k+2G etc.) represent different wave functions with different frequencies and different energies, but they all belong to the same irreducible representation of the translation symmetry. They have the same symmetry behavior. This means that you can mix them, like you do with wave functions in chemical bonding. As the energies at k and k+G are generally very different this does not matter much except at the edges of a Brillouin zone. The wave function at k=1/2 and k=1/2-1 = -1/2 have the same energy and so mixing will split them up and cause a gap (like the two 1s states of two adjacent H atoms leading to a bonding and an antibonding sigma orbital). This splitting is what causes semiconductors to have an energy gap.

Another way of saying this is to say that the functions at k, k-G (or k+G or k+2G) are aliases of each other. This is particularly important for digital sampling.
 

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