Understanding the concept of Polar and Non-Polar Semiconductors

Apolo
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I don't understand the concept for polar and non-polar semiconductors, generally speaking about propagation of existence of phonons (acustic or optics).

Thanks.
I don't find any thread about this concepts.
 
I don't know too much about this. The classical semiconductors like Si or Ge crystallize in a diamond structure, with two symmetry equivalent atoms per primitive unit cell. In semiconductors like GaAs or ZnS, there are two different atoms with different electronegativity in that unit cell hence the material can easily be polarized and especially the dispersion relation for phonons may be considerably different from that in non-polar materials due to the interaction of the atomic vibrations with electromagnetic radiation. The combined electronic and vibrational excitation is called a polariton.
See e.g. fig. 9.9 in
http://books.google.de/books?id=ZJz...ge&q=phonon dispersion polar crystals&f=false
 
Hi. I have got question as in title. How can idea of instantaneous dipole moment for atoms like, for example hydrogen be consistent with idea of orbitals? At my level of knowledge London dispersion forces are derived taking into account Bohr model of atom. But we know today that this model is not correct. If it would be correct I understand that at each time electron is at some point at radius at some angle and there is dipole moment at this time from nucleus to electron at orbit. But how...
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