Number of electrons in conduction band

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SUMMARY

The discussion focuses on calculating the number of electrons in the conduction band using the density of states function g_c(E) and the Fermi probability distribution f(E). It establishes that the number of electrons between energy levels E and E + dE is given by the equation n(E)dE = g_c(E) f(E) dE. The conversation clarifies that all degenerate states at the same energy level have the same occupancy probability f(E), regardless of spin, as long as there is no symmetry breaking. This results in a factor of 2 in the density of states for spin up and spin down electrons.

PREREQUISITES
  • Understanding of Fermi-Dirac statistics
  • Knowledge of density of states in solid-state physics
  • Familiarity with quantum mechanics principles
  • Basic concepts of electron spin and degeneracy
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  • Study the derivation of the density of states function g_c(E) in semiconductors
  • Explore the implications of symmetry breaking on Fermi-Dirac distribution
  • Learn about the effects of temperature on the Fermi probability distribution f(E)
  • Investigate the role of electron spin in conduction band occupancy
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Physicists, materials scientists, and electrical engineers interested in semiconductor physics and the behavior of electrons in conduction bands.

EmilyRuck
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Hello!
In order to obtain the number of actual electrons in the conduction band or in a range of energies, two functions are needed:
1) the density of states for electrons in conduction band, that is the function g_c(E);
2) the Fermi probability distribution f(E) for the material at its temperature T.
(as a reference, http://ecee.colorado.edu/~bart/book/carriers.htm can be used). So, the number of electrons between the energy level E and the energy level E + dE is given by

n(E)dE = g_c(E) f(E) dE

where g_c(E) dE is the number of states between energy level E and energy level E + dE and f(E) is the probability that they are occupied.
This would work if the number of states in that range is just 1 or 0. But what if there are multiple available states?

Fermi probability distribution gives the probability that a state at a certain energy E is occupied: it is just one state. If we need to handle multiple states (like two electrons with opposite spin) at the same energy (or in the same infinitesimal interval of energies, between E and E + dE), how should we use the value of the Fermi probability for each of them?
 
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Shouldn't degenerate states be taken care of in the density of states? For spin up and spin down, a factor of 2 is included in the density of states, and doesn't affect the Fermi-Dirac distribution.
 
Vagn said:
Shouldn't degenerate states be taken care of in the density of states? For spin up and spin down, a factor of 2 is included in the density of states, and doesn't affect the Fermi-Dirac distribution.

Yes, a factor of 2 is included in the density of states. My question is: if an energy level E_1 is such that (for example) f(E_1) = 0.1 and there are two possible states with opposite spins for the electrons at E = E_1: will both the states have the same 0.1 probability of being occupied? Or what else?
 
EmilyRuck said:
Yes, a factor of 2 is included in the density of states. My question is: if an energy level E_1 is such that (for example) f(E_1) = 0.1 and there are two possible states with opposite spins for the electrons at E = E_1: will both the states have the same 0.1 probability of being occupied? Or what else?
All degenerate states with energy E have the same probability of being occupied, namely f(E), no matter what the spin is.
 
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Fermi-Dirac distribution f(E) gives the probability that a quantum state with energy E is occupied. So, as long as there is no symmetry breaking that lifts the degeneracy of spin up and spin down electrons, they have the same energy, thereore f(E) for spin up and spin down electrons are the same. That's why we have a factor of two. Furthermore, if there are more available states with the same energy, f(E) for all those states would be the same.
 
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Ok, that's right now, so thank you both!
 

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