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In electronics and
semiconductor A semiconductor is a material which has an electrical conductivity value falling between that of a conductor, such as copper, and an insulator, such as glass. Its resistivity falls as its temperature rises; metals behave in the opposite way. ...
physics, the law of mass action is a relation about the concentrations of free electrons and
electron hole In physics, chemistry, and electronic engineering, an electron hole (often simply called a hole) is a quasiparticle which is the lack of an electron at a position where one could exist in an atom or atomic lattice. Since in a normal atom or ...
s under
thermal equilibrium Two physical systems are in thermal equilibrium if there is no net flow of thermal energy between them when they are connected by a path permeable to heat. Thermal equilibrium obeys the zeroth law of thermodynamics. A system is said to be in ...
. It states that, under
thermal equilibrium Two physical systems are in thermal equilibrium if there is no net flow of thermal energy between them when they are connected by a path permeable to heat. Thermal equilibrium obeys the zeroth law of thermodynamics. A system is said to be in ...
, the product of the free electron concentration n and the free hole concentration p is equal to a constant square of intrinsic carrier concentration n_. The intrinsic carrier concentration is a function of temperature. The equation for the mass action law for
semiconductor A semiconductor is a material which has an electrical conductivity value falling between that of a conductor, such as copper, and an insulator, such as glass. Its resistivity falls as its temperature rises; metals behave in the opposite way. ...
s is: np = n_^


Carrier concentrations

In semiconductors, free electrons and holes are the carriers that provide conduction. For cases where the number of carriers are much less than the number of band states, the carrier concentrations can be approximated by using
Boltzmann statistics Ludwig Eduard Boltzmann (; 20 February 1844 – 5 September 1906) was an Austrian physicist and philosopher. His greatest achievements were the development of statistical mechanics, and the statistical explanation of the second law of thermodyn ...
, giving the results below.


Electron concentration

The free-electron concentration ''n'' can be approximated by n = N_c \exp\left \frac\right where * ''E''c is the energy of the
conduction band In solid-state physics, the valence band and conduction band are the bands closest to the Fermi level, and thus determine the electrical conductivity of the solid. In nonmetals, the valence band is the highest range of electron energies in ...
, * ''E''F is the energy of the
Fermi level The Fermi level of a solid-state body is the thermodynamic work required to add one electron to the body. It is a thermodynamic quantity usually denoted by ''µ'' or ''E''F for brevity. The Fermi level does not include the work required to remov ...
, * ''k''B is the
Boltzmann constant The Boltzmann constant ( or ) is the proportionality factor that relates the average relative kinetic energy of particles in a gas with the thermodynamic temperature of the gas. It occurs in the definitions of the kelvin and the gas consta ...
, * ''T'' is the absolute temperature in
kelvin The kelvin, symbol K, is the primary unit of temperature in the International System of Units (SI), used alongside its prefixed forms and the degree Celsius. It is named after the Belfast-born and University of Glasgow-based engineer and ph ...
s, * ''N''c is the effective density of states at the conduction band edge given by N_c = 2\left(\frac\right)^, with ''m*''e being the electron effective mass and ''h'' being Planck's constant.


Hole concentration

The free-hole concentration ''p'' is given by a similar formula p = N_v \exp\left \frac\right where * ''E''F is the energy of the
Fermi level The Fermi level of a solid-state body is the thermodynamic work required to add one electron to the body. It is a thermodynamic quantity usually denoted by ''µ'' or ''E''F for brevity. The Fermi level does not include the work required to remov ...
, * ''E''v is the energy of the
valence band In solid-state physics, the valence band and conduction band are the bands closest to the Fermi level, and thus determine the electrical conductivity of the solid. In nonmetals, the valence band is the highest range of electron energies in ...
, * ''k''B is the
Boltzmann constant The Boltzmann constant ( or ) is the proportionality factor that relates the average relative kinetic energy of particles in a gas with the thermodynamic temperature of the gas. It occurs in the definitions of the kelvin and the gas consta ...
, * ''T'' is the absolute temperature in
kelvin The kelvin, symbol K, is the primary unit of temperature in the International System of Units (SI), used alongside its prefixed forms and the degree Celsius. It is named after the Belfast-born and University of Glasgow-based engineer and ph ...
s, * ''N''v is the effective density of states at the valence band edge given by N_v = 2\left(\frac\right)^, with ''m*''h being the hole effective mass and ''h'' Planck's constant.


Mass action law

Using the carrier concentration equations given above, the mass action law can be stated as np = N_c N_v \exp\left(-\frac\right) = n_i^2, where ''E''g is the
band gap energy In solid-state physics, a band gap, also called an energy gap, is an energy range in a solid where no electronic states can exist. In graphs of the electronic band structure of solids, the band gap generally refers to the energy difference ...
given by ''E''g = ''E''c − ''E''v. The above equation holds true even for lightly doped extrinsic semiconductors as the product np is independent of
doping Doping may refer to: * Doping, adding a dopant to something * Doping (semiconductor), intentionally introducing impurities into an extremely pure semiconductor to change its electrical properties * Aircraft dope, a lacquer that is applied to fabr ...
concentration.


See also

* Law of mass action


References


External links


Doping, Carrier Concentration, Mobility, and Conductivity

Semi-conductor tutorial
Electronic engineering Empirical laws {{Electronics-stub