Mott VR Hopping Calculation Question

In summary, the Mott 3-D variable range hopping conduction model uses the energy difference between hopping sites, represented by ΔE ≈ 1 / g0rD, to explain conductivity in materials. The g0 in this equation represents the density of states near the Fermi surface and can be calculated as G(E)/V, where G(E) is the DOS and V is the volume. However, this value may vary depending on disorder and there is no known table for reference. The value of ΔE may also vary depending on the material and sample, making it difficult to fit conductivity curves to this model. A general equation cannot be easily derived and may require manipulation of parameters for a good fit.
  • #1
mesogen
25
0
I hope someone out there can help me with this fairly simple but specific question about the Mott 3-D variable range hopping conduction model.

Mott theory has the energy difference between hopping sites as:

ΔE ≈ 1 / g0rD

Where g0 density of states near the Fermi surface, D is the dimension of hopping (1,2,3) and r is the distance between hopping sites.

My question is about using this numerically. I don't know how to calculate or look up a specific number for g0 for a particular material. Also, what are the units of this quantity usually? States/volume? Energy/volume? The second makes sense because the units work out for 3D, but is that the usual unit of density of states?
 
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  • #2
You can define the DOS as just [itex] G(E) = \sum_{i} \delta(E-E_i) [/itex] in which case the units are one over energy. However, in a large system, [itex] G(E) [/itex] diverges with system size, so it makes more sense to define the DOS per unit volume (sometimes also just called the DOS) [itex] g(E) = G(E)/V [/itex]. Obviously this has units of one over (volume times energy).

Especially in a localized phase g(E) makes more physical sense since it as a local measure of the energy level spacing. If you're looking to mix states using an operator that acts within a range [itex] \xi [/itex], then the typical level spacing [itex] \Delta E(\xi) [/itex] of the states mixed by that operator would be roughly [itex] \frac{1}{\Delta E(\xi)} = g(E) \xi^d [/itex]. In other words, to find two states with a splitting much smaller than this you would typically need to look over a larger region.

Unfortunately, I don't know of a place to look up values for this quantity. It's not clear that such a table can even exist since the value may depend on disorder. Nevertheless, you can relate this quantity to a number of other experimentally relevant quantities (not just the hopping conductivity), so that might be an avenue to investigate.

Sorry I couldn't be more helpful.
 
  • #3
Not at all. That was very helpful. It makes me realize that there is nothing that straightforward about VR hopping, even though to me it seems like a relatively simple concept. I'm definitely not a solid state physicist, just a lowly chemist delving into solid state stuff.

The thing is, all I'm trying to do is fit the conductivity over temperature of a certain material (semiconductor, of course) to a model. It certainly doesn't fit the Arrhenius model. It's fairly close to Mott 3D VR hopping, but not good enough. When I try to look up how others fit their curves to this model, there is a great deal of variation, but not much explanation as to how they arrived at their fit.

Anyway, based on your explanation, it seems that ΔE ≈ 1 / g0rD refers to a very local density of states and only deals with two specific hopping points and shouldn't be used as a general statement over the bulk of the material. Generally speaking is there a large difference in ΔE between various different hopping sites over the bulk of the material? Or can one value of ΔE be a good approximation of all the other ones? I guess there would be differences depending on the material and even the sample, but maybe the range is small no matter what?

I guess I'm just looking for a convenient general equation that I can plug into the plotting software, monkey around with some parameters, and fit the curve. It looks like it's not going to be that easy.
 

What is a Mott VR Hopping Calculation?

A Mott VR Hopping Calculation is a theoretical calculation used to determine the hopping rate of particles in a Mott insulator, which is a type of material that does not conduct electricity at low temperatures. It is based on the Mott-Hubbard model, which describes the behavior of electrons in these materials.

Why is understanding Mott VR Hopping important?

Understanding Mott VR Hopping is important because it helps us to understand the properties of materials at low temperatures, and can also be useful in the development of new electronic devices and technologies.

How is a Mott VR Hopping Calculation performed?

A Mott VR Hopping Calculation is performed using mathematical equations and computer simulations. These calculations take into account factors such as the energy levels of the particles and the interactions between them.

What are the applications of Mott VR Hopping Calculations?

Mott VR Hopping Calculations have a wide range of applications, including in the study of superconductors, magnetic materials, and semiconductors. They are also used in the development of electronic devices such as transistors and solar cells.

What are the limitations of Mott VR Hopping Calculations?

One limitation of Mott VR Hopping Calculations is that they are based on simplified models and may not accurately reflect the complexities of real materials. They also require a significant amount of computational power and may not be feasible for very large systems.

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