**Fermi Dirac Function in Semiconductor:**

It is important to know what energies are possessed by a mobile carrier in a solid or semiconductor. This relationship is referred to as **energy distribution function. **We are concerned with the distribution of energy of the free electrons in a metal. The Fermi Dirac Function statistics enables us to find the number of free electrons dn_{E} per unit volume, within energy range E to E + dE at temperature T.

The number of free electrons per cubic metre of a metal whose energies lie in the interval E to E + dE is given by

where dn_{E} represents the number of free electrons per cubic metre whose energies lie in the energy interval dE, and ρ_{E} represents the density of electrons in the energy interval dE.

In case of free electrons, it can be safely assumed that there is no potential variation within the metal. Accordingly, each cubic metre of the metal must have the same number of electrons. That is, the density in space (electrons/m^{3}) is a constant. However, within each unit volume of metal there will be electrons having all possible energies. It is this distribution in energy that is represented by ρ_{E}. ρ_{E} represents the number of electrons per eV per m^{3} of the metal. The function ρ_{E} may be expressed as

where N(E) is the density of states (number of states per eV per cubic metre) in the conduction band, and f(E) is the probability that a quantum state with energy E is occupied by an electron.

The density of states, N(E) is found to be proportional to the half power of energy i.e.,

where γ is a proportionality constant and is defined as

where m is the mass of electron in kg, and h is Planck’s constant in joule-seconds.

The dimensions of γ are (m^{-3}) (eV)^{-3/2}.

The equation for f(E) is known as **Fermi Dirac probability function**, and specifies the fraction of all states at energy E (electron volts) occupied under conditions of thermal equilibrium.

According to the principle of quantum mechanics, the Fermi Dirac probability function is given by

where k is Boltzmann’s constant (k = 8.62 x 10^{-5} eV/K). The function f(E), the Fermi Dirac distribution function, gives the probability that an available energy state at E will be occupied by an electron at absolute temperature T. The quantity E_{F} is called the **Fermi level**, and it represents an important quantity in the analysis of semiconductor behavior. We notice that, for an energy E equal to the Fermi level energy E_{F}, the occupation probability is

Thus an energy state at the Fermi level has a probability of 50 per cent of being occupied by an electron.

A plot of f(E) versus E – E_{F} is depicted in Fig. 6.11 (a) and of E – E_{F} versus f(E) in Fig. 6.11 (b), both for T = 0 K, and for larger values of temperature.

A closer examination of f(E) indicates that at 0 K the distribution takes the simple rectangular form depicted in Fig. 6.12. With T = 0 in the denominator of the exponent, f(E) is 1/1+0 = 1 when the exponent is negative (E < E_{F}), and is 1/1+∞ = 0 when the exponent is positive (E > E_{F}). This rectangular distribution implies that at 0 K every available energy state up to E_{F} is filled up with electrons, and all states above E_{F} are empty.

From Eqs. (6.3), (6.4) and (6.6), we have at absolute zero temperature

At temperatures higher than 0 K, some probability exists for states above the Fermi level to be filled. For example, at T = T_{1} in Fig. 6.12, there is some probability f(E) that states above E_{F} are filled, and there is a corresponding probability [1 – f(E)] that states below E_{F} are empty. The Fermi Dirac function is symmetrical about E_{F} for all temperatures; that is, the probability f(E_{F} + ΔE) that a state ΔE above E_{F} is filled is the same as the probability [1 – f(E_{F} + ΔE)] that a state ΔE below E_{F} is empty. The symmetry of the distribution of empty and filled states about E_{F} makes the Fermi level a natural reference point in calculations of electron and hole concentrations in semiconductors.

**The Fermi Level: **An expression for E_{F} can be had from energy distribution curve depicted in Fig. 6.13 at 0 K. The area under the curve represents the total number of free electrons (per cubic metre of metal). Thus

Substituting γ = 6.82 x 10^{27} from Eq. (6.5), we have

The density n varies from metal to metal, therefore, E_{F} will vary from metal to metal. The density of electrons n and so E_{F}** **may be determined by knowing the specific gravity, the atomic weight, and the number of free electrons per atom. For most of the metals, the numerical value of E_{F}** **is less than 10 eV.