EmilyRuck
- 134
- 6
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?
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?