What is the expression for the density of states in 2D?

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Homework Help Overview

The discussion revolves around finding an expression for the density of states of free two-dimensional electrons as a function of energy. Participants are exploring the relationship between states in k-space and energy, specifically in a two-dimensional context.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to derive the density of states by relating the number of states per unit area of k-space to energy. They express uncertainty in finding the number of states as a function of wave number, N(k).
  • Some participants question the relationship between wavenumbers and energy, suggesting a grid representation of states and exploring how to count states within a given area.
  • Others suggest finding expressions for N(n), N(k), and N(E) sequentially, while also discussing the implications of the area of a circle in k-space.
  • Concerns are raised about the dependence of the density of states on energy and the interpretation of volume in the context of density of states.

Discussion Status

The discussion is active, with participants providing insights and suggestions for approaching the problem. There is recognition of the complexity involved in relating different variables and the need for further exploration of the expressions for N(k) and N(E). Some guidance has been offered, but no consensus has been reached regarding the final expression for the density of states.

Contextual Notes

Participants are working under the constraints of a two-dimensional system and are discussing the implications of quantum mechanics on the density of states. There is an ongoing examination of the definitions and relationships between variables in k-space and energy.

jeebs
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Hi,
I am trying to find an expression for the density of states of free two-dimensional electrons, as a function of energy, and I am really struggling.

I get that what I am looking for is the number of states per unit area of k-space per unit energy, and in general (3D), this is expressed as

density of states g(E) = \frac{1}{V}\frac{dN}{dE}

However, since this is in 2D, the V is actually an area. In k-space, I think a unit of area is A=\frac{\pi}{L}\frac{\pi}{L} = \frac{\pi^2}{L^2} sincek=\frac{\pi}{L} for the smallest allowed length in k-space.

So, what I need is some expression for the number of states, N(E), but presumably have to find it in terms of N(k) first.

So, what I said was that the free electron has energy E = \frac{\hbar^2}{2m_e}(k_x^2 + k_y^2) so that when I know N in terms of k, I can easily convert it to N in terms of E.

So I think I eventually need to get g(E) = \frac{L^2}{\pi^2}\frac{dN(E)}{dE}

However, this is where I have ran out of steam. I haven't been able to come up with an expression for the number of states as a function of wave number, N(k).

Can anyone give me a hand here? It would make a lovely Christmas present :wink:
Cheers.
 
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Well, the actual wavenumbers k_x and k_y of any given state are going to be multiples of the quantum \pi/L, right? (Seriously, correct me if I'm wrong, I'm not 100% sure I'm remembering this correctly) So the energy expression is
E = \frac{\hbar^2\pi^2}{2 m_e L^2}\bigl(n_x^2 + n_y^2\bigr)
Now you have a grid, basically, in which there is a state at each point with integer coordinates. You can make a one-to-one correspondence between points/states and 1x1 unit squares on the grid. So the number of unit squares within any large enough area is about the same as the number of states within that area.

Try finding an expression for N(n), then convert it to N(k), then to N(E). If you're still stuck after a while, I'm sure someone will get back to you.
 
Have you tried writing to Santa? :-p

How many states are inside a circle with radius k?
 
a circle of radius k has an area A=\pi k^2

and i believe there is one state per unit area on that grid, right?

so is the number of states N = \frac{A}{ \pi ^2/L^2} = \frac{L^2k^2}{\pi} ??
 
Seems reasonable so far...
 
Right so, N(k) = \frac{A}{\pi ^2 / L^2} and E = \frac{\hbar ^2k^2}{2m} =\frac{\hbar ^2n^2\pi ^2}{2mL^2}

so N(E) = \frac{\pi k^2}{\pi ^2 / L^2} = \frac{L^2}{\pi}\frac{2mE}{\hbar ^2}

so my density of states is given by g(E) = \frac{1}{A}\frac{dN(E)}{dE} = \frac{1}{A}\frac{2mL^2}{\pi \hbar ^2} = \frac{2mL^4}{\pi^3 \hbar ^2} ?


how can this be right if I am looking for g as a function of E, but E does not appear in this expression?
 
The expression before last is correct, I think. However the V in g(E) = \frac{1}{V}\frac{dN}{dE} refers to the volume in position space (volume of the "box") not volume in momentum space. As to E dependence, it seems that for a 2D system the energy density is constant.
 

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