Graphene Energy Dispersion and Density of States: Understanding the Relationship

In summary, the conversation discusses two questions related to 2D graphene. The first question involves determining the number of nearest neighbours in a primitive cell of graphene, while the second question is about determining the density of states for graphene's linear energy dispersion near the fermi level. The equation E=(hbar)vF|k| is used to describe the energy dispersion. The solution involves finding the number of near neighbours to be 3 and nearly proving the required relation. However, an explanation or algebraic proof is still needed for why N=total number of states=(A/2π)∗∫[between 0 and k(E)] dkk in the vicinity of the dirac points. Additionally, it is necessary to show
  • #1
peripatein
880
0
Hi,

Homework Statement


I have two questions, in fact, both involving 2D graphene:
(1) How may I determine the number of nearest neighbours in a primitive cell of graphene?
(2) Given that graphene has linear energy dispersion near the fermi level and the dispersion is given by E=(hbar)vF|k|, I would like to determine the density of states. I think it is equal to g(E)=E/2π[itex](hbar)2vF2, but how may I show that?

I'd appreciate your help.


Homework Equations





The Attempt at a Solution

 
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  • #2
I suppose I will aid in getting the ball rolling with this. There are a number of ways that you can approach this problem, however, it is rather difficult to help you without a gauge on your level of quantum mechanics.
 
  • #3
Hi,
I believe I have managed through most of this. I have found the number of near neighbours to be 3. I even managed to nearly prove the required relation. However, what I am lacking is an explanation, or an algebraic proof, why N=total number of states=(A/2π)∗∫[between 0 and k(E)] dkk in the vicinity of the dirac points?
Also, how may I show that the units of g(E) in the above expression (my first post) are number of states per area per energy?
 

What is graphene?

Graphene is a thin layer of carbon atoms arranged in a hexagonal lattice, just one atom thick. It is considered a "wonder material" due to its unique properties, including its high strength, flexibility, and conductivity.

What is energy dispersion in graphene?

Energy dispersion in graphene refers to the way that electrons move through the material. Due to the unique structure of graphene, electrons behave as if they have no mass and move at extremely high speeds, allowing for efficient energy transfer.

How is graphene used in energy applications?

Graphene has potential uses in various energy applications, such as batteries, solar cells, and supercapacitors. Its high surface area and conductivity make it a promising material for improving energy storage and conversion.

What challenges exist in harnessing graphene for energy purposes?

While graphene has many promising properties for energy applications, there are still challenges that need to be addressed. These include finding ways to produce large quantities of high-quality graphene, improving its stability and durability, and developing cost-effective production methods.

How does energy dispersion in graphene impact its potential for use in electronics?

The unique energy dispersion in graphene allows for the efficient movement of electrons, making it a desirable material for use in electronics. It has the potential to make devices smaller, faster, and more energy-efficient compared to traditional materials.

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