Are Phonon Collisions Responsible for Quantized Lattice Vibrations?

In summary, phonons are quantized lattice vibrations characterized by traveling waves of the form exp(ikr) satisfying periodic boundary conditions. They are also known as normal modes of vibration, which can include standing waves in which all atoms move in phase with each other, or more general modes where atoms oscillate out of phase. Phonon-phonon collisions occur due to the non-linear behavior of the medium, as one phonon changes the configuration of atoms and affects the propagation of the other. These collisions can be best understood in terms of wavepackets, with their energetic width inversely proportional to the width in real space. The number of possible phonon modes is determined by imposing periodic or fixed end boundary conditions on the crystal, which are
  • #1
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Phonons are quantized lattice vibrations. They are traveling waves of the form
exp(ikr) taken to satisfy periodic boundary conditions. I'm guessing periodic boundary conditions are equivalent to demanding the waves to be zero at the boundary. which is what characterizes standing waves (right? :S)
So are all phonons really just the number of possible standing waves you can form from the solutions exp(ikr).
And if so, how is one to interpret phonon-phonon collisions? What happens physically when two standing wave vibrations collide and why can we speak of conservation of the crystal momentum?
 
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  • #2
No. Periodic boundary conditions are the unphysical conditions of requiring the wave function at opposite sides of the box to match each other. It is used for mathematical convenience.

Yes. the phonons are the normal modes of vibration.

Phonons collision happen because of non linear behavior of the medium. One phonon changes the configuration of atoms as it passes by them and the changed configuration affects the propagation of the other phonon.
 
  • #3
So when you say: Yes the phonons are normal modes of vibrations? They are not standing waves in general? (frankly normal mode is not common nomenclature for me)
 
  • #4
Pretty much the same thing. In a standing wave all atoms move in phase with each other. A normal mode is a more general concept which allows for other possibilities where different atoms are oscillating out of phase with each other, but still at the same frequency.
 
  • #5
But surely that kind of exotic behaviour does not happen for plane waves exp(ikr) satisfying the boundary conditions?
And it seems that according to my book these are the only possible phonon modes you can have. At least for calculating the heat capacity these are the only ones considered as contributing - so if you can have all kinds of weird waves which satisfy periodic boundary conditions why is it only the eigenmodes of the system that contribute to the heat capacity?
 
  • #6
The collision of phonons is best considered in terms of wavepackets as any other scattering process.
The energetic width of these wavepackets is inversely proportional to the width of the packets in real space.
As long as this localization length is much smaller than the crystall dimension, the energetic splitting of the sin kx and cos kx standing wave solutions, which is inversely proportional to the crystal dimension L, is negligible and the wavepackets can be considered as being made up of traveling waves exp ikx instead.
This approximation will also break down for very long times during which the wavepackets travel to the crystal boundary and get reflected. But usually, scattering times are much shorter, so that this isn't important either.
 
  • #7
but you too agree that phonons are in general normal modes right? It just seems there is much confusion about the term but this is what I came to conclude.
Also: The possible number of phonon modes are either found by imposing periodic or fixed end boundary conditions on the crystal - why are these procedures equivalent?
 
  • #8
Bulk properties do usually not depend on the boundary conditions chosen in the infinite volume limit. That is why usually periodic boundary conditions (Born - von Karman boundary conditions are chosen). Ashcroft and Mermin has some references on that topic.
 

1. What are phonon collisions?

Phonon collisions are interactions between phonons, which are quasiparticles that represent the collective vibrational modes of atoms in a solid material. These collisions can occur due to various factors such as defects, impurities, and thermal energy, and can affect the propagation of phonons through the material.

2. How do phonon collisions affect thermal conductivity?

Phonon collisions can scatter and redirect the flow of phonons, resulting in a decrease in thermal conductivity. This is because the collisions disrupt the coherent motion of phonons, making it more difficult for them to transport heat through the material.

3. What is the difference between normal and Umklapp phonon collisions?

Normal phonon collisions involve a change in the direction of phonon propagation, while Umklapp collisions involve a change in the phonon's energy and momentum. Umklapp collisions are more likely to occur at higher temperatures and can significantly decrease thermal conductivity.

4. How do phonon collisions affect the electronic properties of a material?

Phonon collisions can also affect the electronic properties of a material by altering the electron-phonon interactions. These interactions can lead to phenomena such as electron-phonon scattering, which can affect the conductivity and other electronic properties of the material.

5. Can phonon collisions be controlled or manipulated?

Yes, phonon collisions can be controlled and manipulated through various methods such as introducing defects or impurities in the material, applying external forces or fields, and engineering the material's structure. This can be useful in designing materials with specific thermal and electronic properties for various applications.

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