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{{Short description|Trace of impurity element that is added to material to alter its electrical or optical properties}}
{{Distinguish|doping in sport}}
{{Distinguish|doping in sport}}
{{About|elemental impurities|the fictional characters in ''[[Kamen Rider W]]''|Dopant (Kamen Rider)}}
{{About|elemental impurities|the fictional characters in ''[[Kamen Rider W]]''|List of Kamen Rider W characters#Dopant}}
{{Refimprove|date=December 2008}}
{{Refimprove|date=December 2008}}


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 [[optics|optical]] properties. The amount of dopant is typically very low compared to the material being doped.
A '''dopant''', also called a '''doping agent''', is a trace impurity element that is inserted into a substance (in very low concentrations) to alter the [[electrical]] or [[optics|optical]] properties of the substance. In the case of [[crystal]]line substances, the atoms of the dopant very commonly take the place of elements that were in the [[crystal lattice]] of the base material. The crystalline materials are frequently either crystals of a [[semiconductor]] such as [[silicon]] and [[germanium]] for use in [[solid-state electronics]], or [[transparency and translucency|transparent]] crystals for use in the production of various [[laser]] types; however, in some cases of the latter, noncrystalline substances such as [[glass]] can also be doped with impurities.


When doped into [[crystal]]line substances, the dopant's atoms get incorporated into the crystal lattice of the substance. The crystalline materials are frequently either crystals of a [[semiconductor]] such as [[silicon]] and [[germanium]] for use in [[solid-state electronics]], or [[transparency and translucency|transparent]] crystals for use in the production of various [[laser]] types; however, in some cases of the latter, noncrystalline substances such as [[glass]] can also be doped with impurities.
==Semiconductors==
{{Main|Doping (semiconductor)}}


In solid-state electronics, using the proper types and amounts of dopants in semiconductors is what produces the [[p-type semiconductor]]s and [[n-type semiconductor]]s that are essential for making [[transistor]]s and [[diode]]s.
In solid-state electronics using the proper types and amounts of dopants in semiconductors is what produces the [[p-type semiconductor]]s and [[n-type semiconductor]]s that are essential for making [[transistor]]s and [[diode]]s.


==Transparent crystals==
The addition of a dopant to a [[semiconductor]], known as [[doping (semiconductor)|doping]], has the effect of shifting the [[Fermi level]]s within the material. This results in a material with predominantly negative ([[n-type semiconductor|n-type]]) or positive ([[p-type semiconductor|p-type]]) [[charge carrier]]s depending on the dopant variety. Pure semiconductors that have been altered by the presence of dopants are known as [[extrinsic semiconductor]]s [See: [[intrinsic semiconductor]]]. Dopants are introduced into semiconductors in a variety of techniques: solid sources, gases, spin on liquid, and ion implanting. See [[ion implantation]], surface [[diffusion]], and solid sources footnote.


==Lasing media==
=== Lasing media ===
The procedure of doping tiny amounts of the metals [[chromium]] (Cr), [[neodymium]] (Nd), [[erbium]] (Er), [[thulium]] (Tm), [[ytterbium]] (Yb), and a few others, into transparent [[crystal]]s, [[ceramic]]s, or [[glass]]es is used to produce the [[Active laser medium|active medium]] for [[solid-state laser]]s. It is in the electrons of the dopant atoms that a [[population inversion]] can be produced, and this population inversion is essential for the [[stimulated emission]] of photons in the operation of ''all'' [[laser]]s.
The procedure of doping tiny amounts of the metals [[chromium]] (Cr), [[neodymium]] (Nd), [[erbium]] (Er), [[thulium]] (Tm), [[ytterbium]] (Yb), and a few others, into transparent [[crystal]]s, [[ceramic]]s, or [[glass]]es is used to produce the [[Active laser medium|active medium]] for [[solid-state laser]]s. It is in the electrons of the dopant atoms that a [[population inversion]] can be produced, and this population inversion is essential for the [[stimulated emission]] of photons in the operation of ''all'' [[laser]]s.


In the case of the natural [[ruby]], what has occurred is that a tiny amount of [[chromium]] dopant has been naturally distributed through a crystal of [[aluminum oxide]] (corundum). This chromium both gives a ruby its red color and also enables a ruby to undergo a population inversion and act as a laser. The aluminum and oxygen atoms in the transparent crystal of aluminum oxide served simply to support the chromium atoms in a good spatial distribution, and otherwise, they do not have anything to do with the laser action.
In the case of the natural [[ruby]], what has occurred is that a tiny amount of chromium dopant has been naturally distributed through a crystal of [[aluminium oxide]] ([[corundum]]). This chromium both gives a ruby its red color, and also enables a ruby to undergo a population inversion and act as a laser. The aluminium and oxygen atoms in the transparent crystal of aluminium oxide served simply to support the chromium atoms in a good spatial distribution, and otherwise, they do not have anything to do with the laser action.


In other cases, such as in the [[Nd:YAG|neodymium YAG laser]], the crystal is synthetically made and does not occur in nature. The man-made [[yttrium aluminum garnet]] crystal contains millions of yttrium atoms in it, and due to its physical size, chemical valence, etc., it works well to take the place of a small minority of yttrium atoms in its lattice, and to replace them with atoms from the [[Rare earth element|rare earth]] series of elements, such as neodymium. Then, these dopant atoms actually carry out the lasing process in the crystal. The rest of the atoms in the crystal consist of yttrium, aluminum, and oxygen atoms, but just as above, these other three elements function to simply support the neodymium atoms. In addition, the rare-earth element erbium can readily be used as the dopant rather than neodymium, giving a different wavelength of its output.
In other cases, such as in the [[Nd:YAG|neodymium YAG laser]], the crystal is synthetically made and does not occur in nature. The human-made [[yttrium aluminium garnet]] crystal contains millions of yttrium atoms in it, and due to its physical size, chemical valence, etc., it works well to take the place of a small minority of yttrium atoms in its lattice, and to replace them with atoms from the [[rare-earth]] series of elements, such as neodymium. Then, these dopant atoms actually carry out the lasing process in the crystal. The rest of the atoms in the crystal consist of yttrium, aluminium, and oxygen atoms, but just as above, these other three elements function to simply support the neodymium atoms. In addition, the rare-earth element erbium can readily be used as the dopant rather than neodymium, giving a different wavelength of its output.


In many [[transparency (optics)|optically-transparent]] hosts, such active centers may keep their excitation for a time on the order of milliseconds, and relax with [[stimulated emission]], providing the laser action. The amount of dopant is usually measured in [[atomic percent]]. Usually the relative atomic percent is assumed in the calculations, taking into account that the dopant ion can substitute in only part of site in a crystalline lattice. The doping can be also used to change the [[refraction index]] in [[optical fiber]]s, especially in the [[double-clad fiber]]s. The optical dopants are characterized with lifetime of excitation and the effective absorption and emission cross-sections, which are main parameters of an active dopant. Usually, the concentration of optical dopant is of order of few percent or even lower. At large density of excitation, the cooperative quenching (cross-relaxation) reduces the efficiency of the laser action.
In many [[transparency (optics)|optically-transparent]] hosts, such active centers may keep their excitation for a time on the order of milliseconds, and relax with [[stimulated emission]], providing the laser action. The amount of dopant is usually measured in [[atomic percent]]. Usually the relative atomic percent is assumed in the calculations, taking into account that the dopant ion can substitute in only part of a site in a crystalline lattice. The doping can be also used to change the [[refraction index]] in [[optical fiber]]s, especially in the [[double-clad fiber]]s. The optical dopants are characterized with lifetime of excitation and the effective absorption and emission cross-sections, which are main parameters of an active dopant. Usually, the concentration of optical dopant is of order of few percent or even lower. At large density of excitation, the cooperative quenching (cross-relaxation) reduces the efficiency of the laser action.

=== Examples ===
The medical field has some use for [[erbium]]-doped laser crystals for the [[laser scalpel]]s that are used in [[laser surgery]]. [[Europium]], [[neodymium]], and other rare-earth elements are used to dope [[glass]]es for lasers. [[Holmium]]-doped and [[Nd:YAG laser|neodymium]] yttrium aluminium garnets (YAGs) are used as the [[active laser medium]] in some laser scalpels.<ref>{{cite journal |last=Moskalik |first=K |author2=A Kozlov |author3=E Demin |author4=E Boiko |year=2009 |title=The Efficacy of Facial Skin Cancer Treatment with High-Energy Pulsed Neodymium and Nd:YAG Lasers |journal=Photomedicine Laser Surgery |volume=27 |issue=2 |pages=345–349 |doi=10.1089/pho.2008.2327 |pmid=19382838}}</ref>


==Phosphors and scintillators==
==Phosphors and scintillators==
In context of [[phosphor]]s and [[scintillator]]s, dopants are better known as [[activator (phosphor)|activator]]s.
In context of [[phosphor]]s and [[scintillator]]s, dopants are better known as [[activator (phosphor)|activator]]s, and are used to enhance the luminescence process.<ref>{{cite book
|first1=N. Thejo |last1=Kalyani |first2=Hendrik |last2=Swart |first3=S.J. |last3=Dhoble |title=Principles and Applications of Organic Light Emitting Diodes (OLEDs) |page=25}}</ref>

== Semiconductors ==
{{Main article|Doping (semiconductor)}}
The addition of a dopant to a [[semiconductor]], known as [[doping (semiconductor)|doping]], has the effect of shifting the [[Fermi level]]s within the material.{{citation needed|date=April 2019}} This results in a material with predominantly negative ([[n-type semiconductor|n-type]]) or positive ([[p-type semiconductor|p-type]]) [[charge carrier]]s depending on the dopant variety. Pure semiconductors that have been altered by the presence of dopants are known as [[extrinsic semiconductor]]s (see [[intrinsic semiconductor]]). Dopants are introduced into semiconductors in a variety of techniques: solid sources, gases, spin on liquid, and ion implanting. See [[ion implantation]], surface [[diffusion]], and solid sources footnote.


== Examples ==
== Others ==
The color of some [[gemstone]]s is caused by dopants. For example, ruby and [[sapphire]] are both aluminium oxide, the former getting its red color from chromium atoms, and the latter doped with any of several elements, giving a variety of colors.
*[[Boron]], [[arsenic]], [[phosphorus]], [[antimony]], among other substances, are commonly used dopants in the semiconductor industry.
**Dopants for [[silicon]] and [[germanium]], [[carbon group|group IV]] semiconductors:
***Donors: [[pnictogen|group V]] atoms: [[antimony]], [[phosphorus]], [[arsenic]]
***Acceptors: [[boron group|group III]] atoms: [[boron]], [[aluminium]], [[gallium]]
**Dopants for [[gallium arsenide]], a group III-V semiconductor:
***Donors: [[chalcogen|group VI]] and [[carbon group|group IV]] atoms: [[sulfur]], [[selenium]], [[tellurium]], [[silicon]], [[germanium]].
***Acceptors: [[alkaline earth metal|group II]] and [[carbon group|group IV]] atoms: [[magnesium]], [[zinc]], [[cadmium]], [[silicon]], [[germanium]]
*The medical field has some use for [[erbium]]-doped laser crystals for the [[laser scalpel]]s that are used in [[laser surgery]]. [[Europium]], [[neodymium]], and other [[rare earth elements]] are used to dope [[glass]]es for lasers. [[Holmium]]-doped and [[Nd:YAG laser|neodymium]] [[yttrium aluminium garnet]]s (YAGs) are used as the [[active laser medium]] in some laser scalpels.<ref>{{cite journal | last = Moskalik | first = K |author2=A Kozlov |author3=E Demin |author4=E Boiko | title = The Efficacy of Facial Skin Cancer Treatment with High-Energy Pulsed Neodymium and Nd:YAG Lasers | journal = Photomedical Laser Surgery | year = 2009 | volume = 27 | issue = 2 | pages = 345–349 | doi = 10.1089/pho.2008.2327 | pmid = 19382838}}</ref>
*The color of some [[gemstone]]s is caused by dopants. For example, [[ruby]] and [[sapphire]] are both [[aluminum oxide]], the former getting its red color from [[chromium]] atoms, and the latter doped with any of several elements, giving a variety of colors.


== See also ==
== See also ==
Line 42: Line 42:


[[Category:Semiconductor properties]]
[[Category:Semiconductor properties]]
[[Category:Materials science]]
[[Category:Physical properties]]
[[Category:Chemical properties]]
[[Category:Crystals]]

Latest revision as of 07:46, 26 January 2024

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. The amount of dopant is typically very low compared to the material being doped.

When doped into crystalline substances, the dopant's atoms get incorporated into the crystal lattice of the substance. The crystalline materials are frequently either crystals of a semiconductor such as silicon and germanium for use in solid-state electronics, or transparent crystals for use in the production of various laser types; however, in some cases of the latter, noncrystalline substances such as glass can also be doped with impurities.

In solid-state electronics using the proper types and amounts of dopants in semiconductors is what produces the p-type semiconductors and n-type semiconductors that are essential for making transistors and diodes.

Transparent crystals

[edit]

Lasing media

[edit]

The procedure of doping tiny amounts of the metals chromium (Cr), neodymium (Nd), erbium (Er), thulium (Tm), ytterbium (Yb), and a few others, into transparent crystals, ceramics, or glasses is used to produce the active medium for solid-state lasers. It is in the electrons of the dopant atoms that a population inversion can be produced, and this population inversion is essential for the stimulated emission of photons in the operation of all lasers.

In the case of the natural ruby, what has occurred is that a tiny amount of chromium dopant has been naturally distributed through a crystal of aluminium oxide (corundum). This chromium both gives a ruby its red color, and also enables a ruby to undergo a population inversion and act as a laser. The aluminium and oxygen atoms in the transparent crystal of aluminium oxide served simply to support the chromium atoms in a good spatial distribution, and otherwise, they do not have anything to do with the laser action.

In other cases, such as in the neodymium YAG laser, the crystal is synthetically made and does not occur in nature. The human-made yttrium aluminium garnet crystal contains millions of yttrium atoms in it, and due to its physical size, chemical valence, etc., it works well to take the place of a small minority of yttrium atoms in its lattice, and to replace them with atoms from the rare-earth series of elements, such as neodymium. Then, these dopant atoms actually carry out the lasing process in the crystal. The rest of the atoms in the crystal consist of yttrium, aluminium, and oxygen atoms, but just as above, these other three elements function to simply support the neodymium atoms. In addition, the rare-earth element erbium can readily be used as the dopant rather than neodymium, giving a different wavelength of its output.

In many optically-transparent hosts, such active centers may keep their excitation for a time on the order of milliseconds, and relax with stimulated emission, providing the laser action. The amount of dopant is usually measured in atomic percent. Usually the relative atomic percent is assumed in the calculations, taking into account that the dopant ion can substitute in only part of a site in a crystalline lattice. The doping can be also used to change the refraction index in optical fibers, especially in the double-clad fibers. The optical dopants are characterized with lifetime of excitation and the effective absorption and emission cross-sections, which are main parameters of an active dopant. Usually, the concentration of optical dopant is of order of few percent or even lower. At large density of excitation, the cooperative quenching (cross-relaxation) reduces the efficiency of the laser action.

Examples

[edit]

The medical field has some use for erbium-doped laser crystals for the laser scalpels that are used in laser surgery. Europium, neodymium, and other rare-earth elements are used to dope glasses for lasers. Holmium-doped and neodymium yttrium aluminium garnets (YAGs) are used as the active laser medium in some laser scalpels.[1]

Phosphors and scintillators

[edit]

In context of phosphors and scintillators, dopants are better known as activators, and are used to enhance the luminescence process.[2]

Semiconductors

[edit]

The addition of a dopant to a semiconductor, known as doping, has the effect of shifting the Fermi levels within the material.[citation needed] This results in a material with predominantly negative (n-type) or positive (p-type) charge carriers depending on the dopant variety. Pure semiconductors that have been altered by the presence of dopants are known as extrinsic semiconductors (see intrinsic semiconductor). Dopants are introduced into semiconductors in a variety of techniques: solid sources, gases, spin on liquid, and ion implanting. See ion implantation, surface diffusion, and solid sources footnote.

Others

[edit]

The color of some gemstones is caused by dopants. For example, ruby and sapphire are both aluminium oxide, the former getting its red color from chromium atoms, and the latter doped with any of several elements, giving a variety of colors.

See also

[edit]

References

[edit]
  1. ^ Moskalik, K; A Kozlov; E Demin; E Boiko (2009). "The Efficacy of Facial Skin Cancer Treatment with High-Energy Pulsed Neodymium and Nd:YAG Lasers". Photomedicine Laser Surgery. 27 (2): 345–349. doi:10.1089/pho.2008.2327. PMID 19382838.
  2. ^ Kalyani, N. Thejo; Swart, Hendrik; Dhoble, S.J. Principles and Applications of Organic Light Emitting Diodes (OLEDs). p. 25.