Intrinsic semiconductor, the Glossary
An intrinsic semiconductor, also called a pure semiconductor, undoped semiconductor or i-type semiconductor, is a semiconductor without any significant dopant species present.[1]
Table of Contents
17 relations: Absolute zero, Charge carrier, Charge carrier density, Crystallographic defect, Dopant, Electrical resistivity and conductivity, Electron, Electron excitation, Electron hole, Excited state, Extrinsic semiconductor, Introduction to Solid State Physics, Mercury cadmium telluride, P–n junction, Semiconductor, Vacancy defect, Valence and conduction bands.
- Semiconductor material types
Absolute zero
Absolute zero is the lowest limit of the thermodynamic temperature scale; a state at which the enthalpy and entropy of a cooled ideal gas reach their minimum value, taken as zero kelvin.
See Intrinsic semiconductor and Absolute zero
Charge carrier
In solid state physics, a charge carrier is a particle or quasiparticle that is free to move, carrying an electric charge, especially the particles that carry electric charges in electrical conductors.
See Intrinsic semiconductor and Charge carrier
Charge carrier density
Charge carrier density, also known as carrier concentration, denotes the number of charge carriers per volume.
See Intrinsic semiconductor and Charge carrier density
Crystallographic defect
A crystallographic defect is an interruption of the regular patterns of arrangement of atoms or molecules in crystalline solids.
See Intrinsic semiconductor and Crystallographic defect
Dopant
A dopant (also called a doping agent) is a small amount of a substance added to a material to alter its physical properties, such as electrical or optical properties.
See Intrinsic semiconductor and Dopant
Electrical resistivity and conductivity
Electrical resistivity (also called volume resistivity or specific electrical resistance) is a fundamental specific property of a material that measures its electrical resistance or how strongly it resists electric current.
See Intrinsic semiconductor and Electrical resistivity and conductivity
Electron
The electron (or in nuclear reactions) is a subatomic particle with a negative one elementary electric charge.
See Intrinsic semiconductor and Electron
Electron excitation
Electron excitation is the transfer of a bound electron to a more energetic, but still bound state.
See Intrinsic semiconductor and Electron excitation
Electron hole
In physics, chemistry, and electronic engineering, an electron hole (often simply called a hole) is a quasiparticle denoting the lack of an electron at a position where one could exist in an atom or atomic lattice.
See Intrinsic semiconductor and Electron hole
Excited state
In quantum mechanics, an excited state of a system (such as an atom, molecule or nucleus) is any quantum state of the system that has a higher energy than the ground state (that is, more energy than the absolute minimum).
See Intrinsic semiconductor and Excited state
Extrinsic semiconductor
An extrinsic semiconductor is one that has been doped; during manufacture of the semiconductor crystal a trace element or chemical called a doping agent has been incorporated chemically into the crystal, for the purpose of giving it different electrical properties than the pure semiconductor crystal, which is called an intrinsic semiconductor. Intrinsic semiconductor and extrinsic semiconductor are semiconductor material types.
See Intrinsic semiconductor and Extrinsic semiconductor
Introduction to Solid State Physics
Introduction to Solid State Physics, known colloquially as Kittel, is a classic condensed matter physics textbook written by American physicist Charles Kittel in 1953.
See Intrinsic semiconductor and Introduction to Solid State Physics
Mercury cadmium telluride
Hg1−xCdxTe or mercury cadmium telluride (also cadmium mercury telluride, MCT, MerCad Telluride, MerCadTel, MerCaT or CMT) is a chemical compound of cadmium telluride (CdTe) and mercury telluride (HgTe) with a tunable bandgap spanning the shortwave infrared to the very long wave infrared regions.
See Intrinsic semiconductor and Mercury cadmium telluride
P–n junction
A p–n junction is a combination of two types of semiconductor materials, p-type and n-type, in a single crystal.
See Intrinsic semiconductor and P–n junction
Semiconductor
A semiconductor is a material that has an electrical conductivity value falling between that of a conductor, such as copper, and an insulator, such as glass.
See Intrinsic semiconductor and Semiconductor
Vacancy defect
In crystallography, a vacancy is a type of point defect in a crystal where an atom is missing from one of the lattice sites.
See Intrinsic semiconductor and Vacancy defect
Valence and conduction bands
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.
See Intrinsic semiconductor and Valence and conduction bands
See also
Semiconductor material types
- Bipolar magnetic semiconductor
- Degenerate semiconductor
- Extrinsic semiconductor
- Intrinsic semiconductor
- Linear chain compound
- Magnetic semiconductor
- Narrow-gap semiconductor
- Organic photorefractive materials
- Organic semiconductor
- Strained silicon
- Wide-bandgap semiconductor
References
[1] https://en.wikipedia.org/wiki/Intrinsic_semiconductor
Also known as I-type semiconductor, Undoped semiconductor.