Charge carrier

Source: Wikipedia, the free encyclopedia.

In

solid state physics.[2] In a conducting medium, an electric field can exert force on these free particles, causing a net motion of the particles through the medium; this is what constitutes an electric current.[3]
The electron and the proton are the elementary charge carriers, each carrying one elementary charge (e), of the same magnitude and opposite sign.

In conductors

In conducting media, particles serve to carry charge:

In some conductors, such as ionic solutions and plasmas, positive and negative charge carriers coexist, so in these cases an electric current consists of the two types of carrier moving in opposite directions. In other conductors, such as metals, there are only charge carriers of one polarity, so an electric current in them simply consists of charge carriers moving in one direction.

In semiconductors

There are two recognized types of charge carriers in

valence band electron population (holes) as a second type of charge carrier, which carry a positive charge equal in magnitude to that of an electron.[12]

Carrier generation and recombination

When an electron meets with a hole, they recombine and these free carriers effectively vanish.[13] The energy released can be either thermal, heating up the semiconductor (thermal recombination, one of the sources of waste heat in semiconductors), or released as photons (optical recombination, used in LEDs and semiconductor lasers).[14] The recombination means an electron which has been excited from the valence band to the conduction band falls back to the empty state in the valence band, known as the holes. The holes are the empty states created in the valence band when an electron gets excited after getting some energy to pass the energy gap.

Majority and minority carriers

The more abundant charge carriers are called majority carriers, which are primarily responsible for

p-type semiconductors they are holes. The less abundant charge carriers are called minority carriers; in n-type semiconductors they are holes, while in p-type semiconductors they are electrons.[15]

In an intrinsic semiconductor, which does not contain any impurity, the concentrations of both types of carriers are ideally equal. If an intrinsic semiconductor is doped with a donor impurity then the majority carriers are electrons. If the semiconductor is doped with an acceptor impurity then the majority carriers are holes.[16]

Minority carriers play an important role in

inversion layer), so conventionally the source and drain designation for the carriers is adopted, and FETs are called "majority carrier" devices.[18]

Free carrier concentration

Free carrier concentration is the

valence band) by doping. Therefore, they will not act as double carriers by leaving behind holes (electrons) in the other band. In other words, charge carriers are particles that are free to move, carrying the charge. The free carrier concentration of doped semiconductors shows a characteristic temperature dependence.[19]

See also

References

  1. ^ Dharan, Gokul; Stenhouse, Kailyn; Donev, Jason (May 11, 2018). "Energy Education - Charge carrier". Retrieved April 30, 2021.
  2. ^ "Charge carrier". The Great Soviet Encyclopedia 3rd Edition. (1970-1979).
  3. ^ Nave, R. "Microscopic View of Electric Current". Retrieved April 30, 2021.
  4. ^ Nave, R. "Conductors and Insulators". Retrieved April 30, 2021.
  5. ^ Fitzpatrick, Richard (February 2, 2002). "Conduction electrons in a metal". Retrieved April 30, 2021.
  6. ^ a b "Conductors-Insulators-Semiconductors". Retrieved April 30, 2021.
  7. ^ Steward, Karen (August 15, 2019). "Cation vs Anion: Definition, Chart and the Periodic Table". Retrieved April 30, 2021.
  8. University of Illinois at Urbana–Champaign. Archived from the original
    on May 15, 2021. Retrieved April 30, 2021.
  9. ^ Souček, Pavel (October 24, 2011). "Plasma conductivity and diffusion" (PDF). Retrieved April 30, 2021.
  10. ^ Alba, Michael (January 19, 2018). "Vacuum Tubes: The World Before Transistors". Retrieved April 30, 2020.
  11. ^ "Cathode Rays | Introduction to Chemistry". Retrieved April 30, 2021.
  12. ^ Nave, R. "Intrinsic Semiconductors". Retrieved May 1, 2021.
  13. ^ Van Zeghbroeck, B. (2011). "Carrier recombination and generation". Archived from the original on May 1, 2021. Retrieved May 1, 2021.
  14. ^ del Alamo, Jesús (February 12, 2007). "Lecture 4 - Carrier generation and recombination" (PDF). MIT Open CourseWare, Massachusetts Institute of Technology. p. 3. Retrieved May 2, 2021.
  15. ^ "Majority and minority charge carriers". Retrieved May 2, 2021.
  16. ^ Nave, R. "Doped Semiconductors". Retrieved May 1, 2021.
  17. ^ Smith, J. S. "Lecture 21: BJTs" (PDF). Retrieved May 2, 2021.
  18. ^ Tulbure, Dan (February 22, 2007). "Back to the basics of power MOSFETs". EE Times. Retrieved May 2, 2021.
  19. ^ Van Zeghbroeck, B. (2011). "Carrier densities". Retrieved July 28, 2022.