Dynamical Matrix of a BCC Lattice

In summary, the conversation discusses finding the dynamical matrix of a bcc lattice with only nearest neighbours, involving equations of motion and a 3x3 matrix with 8 terms. There is confusion about the process and calculations, but it is determined that there should be 9 equations with 6 of them being 0. The matrix elements correspond to movement and restoring forces in different directions, with some elements being 0.
  • #1
Gogsey
160
0
Hi,

So I have to find the dynamical matricx of a bcc lattice considering only nearest neighbours. Its like if the nearest neighbours were all attached to the atom in question by springs.

So first we need the equations of motion for the lattice. There are 8 nearest neighbours, so the equations of motion, which there should be 3 for each dimension, should have 8 terms due to the forces from the 8 neighbours. So we should also have a 3x3 matrix with each element in the matrix being a sum of 8 terms.

I'm just having a little difficulty in picturing what's going on.

So I oriented the x and y-axis so the directly point along 2 of the 4 directions of the neighbours. And the distance between the atoms is root(3)a/2. So I found that, with a little algebra and geometry, that there are 4 coefficients in these equations. I found that they are root(3)/2, root(3/2), 3/2 and 3, but I'm not sure if this is what I should be doing.

These are the coefficients of the forces, or magnitudes of the forces, in the specified direction of each atom, if we orient them as mentioned above. I won't write out the full equations since that would be very messy and difficult to do since there are 3 equations with 8 terms from each neighbour, plus the ma term.. Am I doing it right?
 
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  • #2
Gogsey said:
Hi,

So I have to find the dynamical matricx of a bcc lattice considering only nearest neighbours. Its like if the nearest neighbours were all attached to the atom in question by springs.

So first we need the equations of motion for the lattice. There are 8 nearest neighbours, so the equations of motion, which there should be 3 for each dimension, should have 8 terms due to the forces from the 8 neighbours. So we should also have a 3x3 matrix with each element in the matrix being a sum of 8 terms.

I'm just having a little difficulty in picturing what's going on.

So I oriented the x and y-axis so the directly point along 2 of the 4 directions of the neighbours. And the distance between the atoms is root(3)a/2. So I found that, with a little algebra and geometry, that there are 4 coefficients in these equations. I found that they are root(3)/2, root(3/2), 3/2 and 3, but I'm not sure if this is what I should be doing.

These are the coefficients of the forces, or magnitudes of the forces, in the specified direction of each atom, if we orient them as mentioned above. I won't write out the full equations since that would be very messy and difficult to do since there are 3 equations with 8 terms from each neighbour, plus the ma term.. Am I doing it right?

I'm confused myself. How does one go from the equations of motion to a 3x3 matrix assuming that the BCC lattice has a basis of two atoms? If we take the components x,y,z as if it were a 3-D crystal, would that mean you end up with six equations (3 eqns for each basis)?

Aschroft Mermin is way over my head. Kittel (the required text) doesn't even cover the dynamical matrix approach in three dimensions.
 
  • #3
Turns out there should be 9 equation, but 6 of them are 0.

Rge matris elements are, movement of an atom in x directio, what is the restoring force in x-direction.

This is the same for xy,xz,yx,yy,yz,zx,zy,zz.

xx, yy, zz are down the diagonal of the matrix. the others would be in there positions, but they should be all zero I think.
 

1. What is the Dynamical Matrix of a BCC Lattice?

The Dynamical Matrix of a BCC (Body-Centered Cubic) Lattice is a mathematical representation of the lattice dynamics, which describes the vibrations and movements of atoms within a BCC crystal structure. It is an essential tool for understanding the physical properties of materials, such as thermal and electrical conductivity.

2. How is the Dynamical Matrix of a BCC Lattice calculated?

The Dynamical Matrix is calculated using the force constants, which are the second derivatives of the interatomic potential energy with respect to the atomic positions. These force constants can be obtained from first-principles calculations or experimental measurements, and they are used to construct the Dynamical Matrix through a series of matrix operations.

3. What is the significance of the Dynamical Matrix in materials science?

The Dynamical Matrix provides important information about the vibrational properties of materials, such as the frequencies and modes of lattice vibrations. This information is crucial for understanding the thermal and mechanical behavior of materials, as well as their response to external stimuli like temperature and pressure. It also plays a critical role in the design and development of new materials with desired properties.

4. Can the Dynamical Matrix of a BCC Lattice be used to study defects in materials?

Yes, the Dynamical Matrix can be used to study defects in materials, such as point defects, dislocations, and grain boundaries. By incorporating these defects into the matrix calculations, it is possible to investigate their effects on the lattice dynamics and the overall properties of the material. This is especially important in the study of materials for advanced technologies, where defects can significantly impact performance.

5. Are there any limitations or challenges in using the Dynamical Matrix for materials research?

One of the main challenges in using the Dynamical Matrix is the computational complexity involved in its calculation. This can limit its application to small systems or simple crystal structures. Additionally, the accuracy of the Dynamical Matrix is highly dependent on the quality of the force constants used, which can be difficult to obtain experimentally. However, with advances in computational techniques and materials characterization methods, these limitations can be overcome, making the Dynamical Matrix an indispensable tool in materials research.

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