Dispersion relation diagrams, phonons

In summary, optical phonons in crystals with more than one atom per unit cell can have a non-zero energy at k=0 due to the displacement of atoms relative to each other, allowing for a restoring force and a non-zero value for omega. This is not the case for crystals with only one atom per unit cell.
  • #1
_Andreas
144
1
In dispersion relation diagrams, where omega is plotted against k, omega is sometimes nonzero at k=0. How is this possible? I thought a wave had to have a nonzero wavenumber :confused:
 
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  • #2
Optical phonons have non-zero components at the center of the Brillouin zone.
 
  • #3
The reason this is possible (as Dr T says, the optical branch has non-zero energy at k=0) is because k is not really a wavenumber.

p = [hbar]k is the 'crystal momentum', which is not a real momentum.
 
  • #4
Also, you could easily be reading a reduced zone scheme, in which the band from the next zone is folded back into the first zone.

Zz.
 
  • #5
Optical phonons occur in crystals which have more than one atom per unit cell. If you have a phonon with k=0 that means the displacement of atoms is the same in every cell. When you have only one atom per cell, then a k=0 displacement is just a shift of the whole crystal, so there can't be a restoring force (hence, [tex]\omega=0[/tex]). But if you have more than one atom per unit cell then the atoms could displace relative to one another (eg. like a bond-stretching mode). Then you can have a k=0 wave, where the displacement is the same in each cell, but the atoms in the cell move relative to one another. Then you will have a restoring force, and have [tex]\omega > 0[/tex] for this type of phonon.
 
  • #6
Wow, thanks guys!
 

Related to Dispersion relation diagrams, phonons

What are dispersion relation diagrams?

Dispersion relation diagrams are graphical representations of the relationship between the frequency and wavevector of a wave in a given medium. They are commonly used in physics and engineering to study the propagation of waves, such as light or sound, through a material.

How are dispersion relation diagrams useful in studying phonons?

Phonons are quantized lattice vibrations in a solid material, and their dispersion relation diagrams show the relationship between their frequency and wavevector. These diagrams provide valuable information about the properties of the material, such as its elastic and thermal properties, and can also help in understanding how phonons contribute to thermal conductivity and heat capacity.

What is the difference between an acoustic phonon and an optical phonon?

An acoustic phonon is a type of phonon that involves the collective motion of atoms in a solid, while an optical phonon involves the interaction between phonons and photons. Acoustic phonons are typically low frequency and have a linear dispersion relation, while optical phonons have a higher frequency and exhibit anharmonic behavior in their dispersion relation.

How do you interpret a dispersion relation diagram?

A dispersion relation diagram typically shows the frequency of a wave on the y-axis and the wavevector (or momentum) on the x-axis. The slope of the curve represents the speed of the wave, and the curvature of the curve provides information about the anharmonic behavior of the material. The points where the curve intersects the x-axis (zero frequency) are known as the Brillouin zone boundaries, which define the boundaries of the first Brillouin zone.

Can dispersion relation diagrams be used to study other types of waves besides phonons?

Yes, dispersion relation diagrams can be used to study various types of waves, such as electromagnetic waves, gravitational waves, and even quantum mechanical waves. They are a useful tool for understanding the behavior of waves in different media and can provide valuable insights into the properties of the material being studied.

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