Applied Physics > Solid State Physics > Band Theory
Band Theory
Band theory is a fundamental concept in solid state physics and forms the basis for understanding the electronic properties of materials. It explains how the discrete energy levels of individual atoms evolve into continuous bands of energy levels in a solid, due to the interactions between a large number of atoms.
Overview:
In isolated atoms, electrons occupy discrete energy levels. However, when atoms come together to form a solid, their outer orbitals overlap, and these discrete levels broaden into energy bands. Band theory describes these continuous bands of energy levels and examines the distribution of electrons within them.
Energy Bands:
The two principal bands critical to band theory are the valence band and the conduction band. The valence band is the highest range of electron energies in which electrons are normally present at absolute zero temperature. The conduction band, on the other hand, is the range of electron energies higher than the valence band, which becomes populated with electrons that contribute to electrical conduction.
Band Gap:
The band gap (\(E_g\)) is the energy difference between the valence band and the conduction band. The magnitude of this band gap is crucial in determining the electrical properties of the material:
- Insulators: Have a large band gap (\(E_g > 4 \text{ eV}\)), preventing electrons from easily moving to the conduction band.
- Semiconductors: Have a moderate band gap (\(0 < E_g < 4 \text{ eV}\)), allowing for electron flow under certain conditions, such as thermal excitation or doping.
- Conductors: Have overlapping valence and conduction bands or a very small band gap, facilitating free movement of electrons.
Mathematical Expression:
The relationship between energy (\(E\)), wave vector (\(k\)), and the effective mass (\(m^*\)) of an electron in a crystal lattice can be described by the nearly-free electron model. In this approximation, the energy dispersion relation for an electron is given by:
\[ E(\mathbf{k}) = \frac{\hbar^2 \mathbf{k}2}{2m*} \]
where \(\hbar\) is the reduced Planck’s constant and \(\mathbf{k}\) is the wave vector of the electron.
Density of States:
The density of states (DOS) function \( g(E) \) describes the number of electronic states per unit energy range at a given energy \( E \). For a three-dimensional non-interacting electron gas, it is given by:
\[ g(E) = \frac{(2m^*){3/2}}{2\pi2 \hbar^3} \sqrt{E - E_c} \]
where \(E_c\) is the conduction band minimum.
Applications:
Band theory is essential for the understanding and development of a wide range of materials and devices, including semiconductors, insulators, and metals. It is particularly significant in the fields of electronics and optoelectronics, where it is used to design transistors, solar cells, LEDs, and many other devices.
In summary, band theory provides a microscopic explanation for the macroscopic electrical properties of materials by considering the collective behavior of electrons within energy bands. This theory is pivotal in applied physics and materials science, enabling the continual advancement of technology.