Umklapp Scattering & Conservation of Energy

Click For Summary
SUMMARY

This discussion focuses on Umklapp scattering, specifically addressing the conservation of momentum and energy during phonon collisions. It is established that momentum is not conserved in certain phonon interactions due to the transfer of reciprocal lattice vectors to the crystal lattice, described by the equation h-bar(k1+k2)=h-bar(k3 + G). While energy is transferred to the lattice, the overall energy remains conserved, as the distribution of phonons follows a Boltzmann distribution during thermalization. The distinction between real momentum and crystal momentum is crucial, as phonons do not carry real momentum, ensuring that energy conservation is maintained throughout the process.

PREREQUISITES
  • Understanding of Umklapp scattering principles
  • Knowledge of phonon interactions in solid-state physics
  • Familiarity with crystal momentum vs. real momentum concepts
  • Basic grasp of thermalization processes in materials
NEXT STEPS
  • Study the mathematical framework of Umklapp scattering in solid-state physics
  • Explore the implications of phonon interactions on thermal conductivity
  • Investigate the Boltzmann distribution in the context of phonon energy states
  • Learn about the role of reciprocal lattice vectors in crystal dynamics
USEFUL FOR

Physicists, materials scientists, and researchers in solid-state physics who are examining the effects of Umklapp scattering on energy and momentum conservation in crystalline materials.

The Head
Messages
137
Reaction score
2
After looking at Umklapp scattering, I believe I have finally gotten most of it down, but a few things are still not clear.

1) Momentum is not conserved for certain phonon collisions, and a certain number of reciprocal lattice vectors are transferred to the crystal lattice:

h-bar(k1+k2)=h-bar(k3 + G)

But if momentum is transferred to the lattice, which is called the thermalization of the lattice, isn't energy transferred to the lattice as well?

2) And if energy is transferred to the lattice. Why would the energy of the phonons still be conserved? It seems to me I am missing something.

3) If the lattice is "thermalized," what exactly is the consequence of this? Does it heat up/dissipate heat, similar to what happens with electrical resistance.
 
Physics news on Phys.org
Yes, the missing energy is thermalized in the lattice. But the energy that was carried away was carried by a phonon ... so phonon energy was conserved at the point of the u-event.
 
  • Like
Likes   Reactions: 1 person
The Head said:
1) Momentum is not conserved for certain phonon collisions, and a certain number of reciprocal lattice vectors are transferred to the crystal lattice:
It seems to me I am missing something.

In deed. You have to be carefull to distinguish real momentum from crystal momentum. Phonons don't carry real momentum at all.
On the other hand, e.g. absorption of a photon will change the momentum of a crystal by a very small amount p. If the total lattice was at rest (i.e. its energy E=0), the energy carried by the lattice afterwards will be ##E=p^2/M ##. As M is practically infinitely large, E=0 even afterwards.
So conservation of real momentum is never a problem and does not interfere with energy conservation.
In the process of thermalization, the total energy remains conserved. However the distribution of the single phonons becomes Boltzmann.
 
  • Like
Likes   Reactions: 1 person

Similar threads

  • · Replies 9 ·
Replies
9
Views
5K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 16 ·
Replies
16
Views
4K
  • · Replies 11 ·
Replies
11
Views
18K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 30 ·
2
Replies
30
Views
3K
  • · Replies 21 ·
Replies
21
Views
2K
Replies
2
Views
2K
  • · Replies 14 ·
Replies
14
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K