Dispersion Relations (tight binding energy)

In summary: Now, at the L point, x = y = z = 0.5. Substituting these values into the equation, we get:E(0.5; 0.5; 0.5) = Ei - A - 8t[cos(pi*0.5)cos(pi*0.5) + cos(pi*0.5)cos(pi*0.5) + cos(pi*0.5)cos(pi*0.5)]= Ei - A - 8t[0 + 0 + 0]= Ei - AThis gives us another endpoint for our sketch. Now, we can connect these two points with
  • #1
cobi18
2
0
The nearest neighbour tight-binding energy band for an fcc metal can be written as:
E(kx; ky; kz) = Ei - A - 8t[cos(pi*kx)cos(pi*ky) + cos(pi*ky)cos(pi*kz) + cos(pi*kz)cos(pi*kx)]where kx; ky; kz are express in units of 2*pi/a .
Sketch this band dispersion (a) between the (capital Gamma) point (kx = ky = kz = 0) and the X point
(kx = 1; ky = kz = 0) (located on the square face of the Brillouin zone), and (b) between
the point and the L point (kx = ky = kz = 1=2) (located on the hexagonal face of the
Brillouin zone).I am not sure even how to start the sketch of this, do I need to know Ei and A, or can I be a lot more simple when just sketching something.

I am just really bad a graphs in reciprocal space, and my lecturer wasn't very helpful.

Any help will be greatly appreciated!
 
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  • #2


Hi there! I can definitely help you with this. Don't worry, you don't need to know the specific values of Ei and A to sketch this band dispersion.

To start, let's define some variables for the sake of simplicity. Let's say kx = x, ky = y, and kz = z. This means that the equation for the energy band becomes:

E(x; y; z) = Ei - A - 8t[cos(pi*x)cos(pi*y) + cos(pi*y)cos(pi*z) + cos(pi*z)cos(pi*x)]

Now, let's look at the two points specified in the forum post: the Gamma point (x = y = z = 0) and the X point (x = 1, y = z = 0).

(a) Sketching between the Gamma point and the X point:
At the Gamma point, all three variables are equal to 0. This means that the energy band becomes:

E(0; 0; 0) = Ei - A - 8t[cos(0)cos(0) + cos(0)cos(0) + cos(0)cos(0)]
= Ei - A - 8t[1 + 1 + 1]
= Ei - A - 24t

This gives us the starting point for our sketch. Now, at the X point, x = 1 and y = z = 0. Substituting these values into the equation, we get:

E(1; 0; 0) = Ei - A - 8t[cos(pi*1)cos(pi*0) + cos(pi*0)cos(pi*0) + cos(pi*0)cos(pi*1)]
= Ei - A - 8t[cos(pi) + 1 + cos(pi)]
= Ei - A - 8t[-1 + 1 - 1]
= Ei - A

This gives us the end point for our sketch. Now, we can simply connect these two points with a curve. The shape of the curve will depend on the values of Ei and A, but it should generally look like a downward sloping curve.

(b) Sketching between the Gamma point and the L point:
At the Gamma point, all three variables are equal to 0. This gives us the same
 

Related to Dispersion Relations (tight binding energy)

1. What is a dispersion relation in tight binding energy?

A dispersion relation in tight binding energy refers to the relationship between the energy of an electron in a solid material and its momentum. It describes how the energy of the electron changes as its momentum varies.

2. How is a dispersion relation calculated?

A dispersion relation can be calculated using mathematical models such as the tight binding approximation, which considers the interaction between electrons and the atomic lattice of a solid material. The dispersion relation is typically represented graphically as a band structure plot.

3. What information can be obtained from a dispersion relation?

A dispersion relation provides important information about the electronic properties of a solid material. It can reveal the energy levels available to electrons, the nature of their motion, and the behavior of the material under different conditions such as temperature and pressure.

4. How does the dispersion relation differ for different materials?

The dispersion relation is unique for each material and depends on factors such as the crystal structure, bonding forces, and electron-electron interactions. Materials with different properties will have distinct band structures and dispersion relations.

5. What applications does the dispersion relation have in science and engineering?

The dispersion relation is a fundamental concept in condensed matter physics and is used to understand and predict the behavior of materials in a variety of fields, including electronics, optics, and materials science. It is also essential in the development of new materials with specific electronic properties.

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