How Does Dimensionality Affect Phonon Polarizations?

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SUMMARY

The discussion centers on the impact of dimensionality on phonon polarizations, specifically transitioning from three dimensions (3D) to two dimensions (2D). In 3D, elastic waves exhibit three polarizations: two transverse and one longitudinal. When moving to 2D, the number of polarizations decreases, leading to two polarizations remaining. The integration factors change from 1/8 in 3D to 1/4 in 2D, and the spherical coordinate term 4πn² simplifies to 2πn in polar coordinates. The discussion concludes that electromagnetic modes retain two polarizations regardless of dimensionality.

PREREQUISITES
  • Understanding of phonon polarizations in solid-state physics
  • Familiarity with dimensional analysis in physics
  • Knowledge of Debye approximation for heat capacity calculations
  • Basic grasp of electromagnetic wave theory
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  • Study the Debye model for heat capacity in 2D systems
  • Explore the implications of dimensionality on wave propagation
  • Research the behavior of electromagnetic modes in various dimensions
  • Investigate the mathematical transition from spherical to polar coordinates in integrals
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Physicists, materials scientists, and students studying solid-state physics, particularly those interested in the effects of dimensionality on wave phenomena and heat capacity in crystalline structures.

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Homework Statement
Consider a crystal made up of two-dimensional layers of atoms, with rigid coupling between the layers. You may assume the motion of atoms is restricted to the plane of the layer. Calculate the phonon heat capacity in the Debye approximation, and show that the low temperature limit is proportional to ##T^2##.
Relevant Equations
In 3D,
##\sum_n{(...)} = \frac{3}{8}\int4\pi n^2dn(...)##

In 2D,
##\sum_n{(...)} = \frac{a}{4}\int2\pi ndn(...)##

What is ##a##?
When going from 3 to 2 dimensions, I am unsure about how the number of polarizations will be affected.

I know the following though:
The 1/8 factor becomes a 1/4 since we are now integrating over the positive quadrant in 2d rather than the positive octant in 3d.
The ##4\pi n^2## becomes a ##2\pi n## because we moved from spherical coordinates to just polar coordinates.

I am told that in 3D, an elastic wave has three polarizations: two transverse and one longitudinal. Do they remain unchanged in lower dimensions? My guess is that they should become 2. But if we lose a polarization every time we lower dimensions, then a photon gas in one dimension shouldn't exist, but it does since the book has a question about it :)
 
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Kyuubi said:
Homework Statement: Consider a crystal made up of two-dimensional layers of atoms, with rigid coupling between the layers. You may assume the motion of atoms is restricted to the plane of the layer. Calculate the phonon heat capacity in the Debye approximation, and show that the low temperature limit is proportional to ##T^2##.
Relevant Equations: In 3D,
##\sum_n{(...)} = \frac{3}{8}\int4\pi n^2dn(...)##

In 2D,
##\sum_n{(...)} = \frac{a}{4}\int2\pi ndn(...)##

What is ##a##?

When going from 3 to 2 dimensions, I am unsure about how the number of polarizations will be affected.

I know the following though:
The 1/8 factor becomes a 1/4 since we are now integrating over the positive quadrant in 2d rather than the positive octant in 3d.
The ##4\pi n^2## becomes a ##2\pi n## because we moved from spherical coordinates to just polar coordinates.

I am told that in 3D, an elastic wave has three polarizations: two transverse and one longitudinal. Do they remain unchanged in lower dimensions? My guess is that they should become 2. But if we lose a polarization every time we lower dimensions, then a photon gas in one dimension shouldn't exist, but it does since the book has a question about it :)
It's been answered for me. Indeed the number of polarizations goes down. I suppose then that EM modes retain their 2 polarizations regardless of dimension (?)
 

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