Band gap - Revision history

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	<onlyinclude>A '''band gap''' is the distance between the [[valence band]] of [[electron]]s and the [[conduction band]]. Essentially, the band gap represents the minimum [[energy]] ~~that is~~ required to excite an electron up to a state in the conduction band where it can participate in conduction.</onlyinclude><ref name="RE2"/> The lower energy level is the valence band, ~~and thus~~ if a gap exists between this level and the higher energy conduction band, energy must be input for electrons to become free. The size and existence of this band gap allows one to visualize the difference between [[conductor]]s, [[semiconductor]]s, and [[insulator]]s.<ref name="RE1">HyperPhysics. (September 26, 2015). ''Band Theory of Solids'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html </ref> These distances can be seen in diagrams known as ''band diagrams'', shown in Figure 1 below.		<onlyinclude>A '''band gap''' is the distance between the [[valence band]] of [[electron]]s and the [[conduction band]]. Essentially, the band gap represents the minimum [[energy]] required to excite an electron up to a state in the conduction band, where it can participate in conduction.</onlyinclude><ref name="RE2"/> The lower energy level is the valence band, therefore if a gap exists between this level and the higher energy conduction band, energy must be input for electrons to become free. In photovoltaic cells, we get that energy from photons. The size and existence of this band gap allows one to visualize the difference between [[conductor]]s, [[semiconductor]]s, and [[insulator]]s.<ref name="RE1">HyperPhysics. (September 26, 2015). ''Band Theory of Solids'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html </ref> These distances can be seen in diagrams known as ''band diagrams'', shown in Figure 1 below.

	[[File:2000px-Band_gap_comparison.svg.png\|780px\|thumb\|center\|Figure 1. A band gap diagram showing the different sizes of band gaps for conductors, semiconductors, and insulators.<ref>Wikimedia Commons. (September 26, 2015). ''Band Gap Comparison'' [Online]. Available: https://upload.wikimedia.org/wikipedia/commons/thumb/0/0b/Band_gap_comparison.svg/2000px-Band_gap_comparison.svg.png</ref>]]		[[File:2000px-Band_gap_comparison.svg.png\|780px\|thumb\|center\|Figure 1. A band gap diagram showing the different sizes of band gaps for conductors, semiconductors, and insulators.<ref>Wikimedia Commons. (September 26, 2015). ''Band Gap Comparison'' [Online]. Available: https://upload.wikimedia.org/wikipedia/commons/thumb/0/0b/Band_gap_comparison.svg/2000px-Band_gap_comparison.svg.png</ref>]]

	==Band Gap Sizes==		==Band Gap Sizes==
	Figure 1 above illustrates the difference in size of the band gap for insulators, conductors, and semiconductors. The size of this band gap gives the materials some of their distinct properties. In insulators, the electrons in the valence band are separated by a large band gap from the conduction band. This means that there is a large "forbidden" gap in energies preventing electrons from the valence band from jumping up into the conduction band and participating in [[conduction]]. This is provides an explanation for why insulators do not conduct [[electricity]] well.<ref>HyperPhysics. (September 26, 2015). ''Insulator Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c4</ref>		Figure 1 above illustrates the difference in size of the band gap for insulators, conductors, and semiconductors. The size of this band gap gives the materials some of their distinct properties.

	In ~~conductors~~, the valence band ~~overlaps with~~ the conduction band. This ~~overlap causes~~ the valence ~~electrons to be essentially free to move~~ into the conduction band and ~~participate~~ in conduction. ~~Since it is~~ not ~~a full overlap, only a fraction of the valence electrons can move through the material, but this is still enough to make conductors conductive~~.<ref>HyperPhysics. (September 26, 2015). ''~~Conductor~~ Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c6</ref>		In insulators, the electrons in the valence band are separated by a large band gap from the conduction band. This means that there is a large "forbidden" gap in energies preventing electrons in the valence band from jumping up into the conduction band and participating in [[conduction]]. This provides an explanation for why insulators do not conduct [[electricity]] well.<ref>HyperPhysics. (September 26, 2015). ''Insulator Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c4</ref>

	In semiconductors, the gap is small enough that it can be bridged by some sort of excitation - perhaps from the [[Sun]] in the case of [[photovoltaic cell]]s. The gap is essentially some size "in-between" that of a conductor or insulator. In this model, a finite number of electrons are able to reach the conduction band and conduct small amounts of electricity.<ref>HyperPhysics. (September 26, 2015). ''Semiconductor Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c5</ref> The excitation of this electron also allows additional conduction processes to occur as a result of the [[electron hole]] left behind. An electron from an atom close by can occupy this space, creating a chain reaction of holes and electron movement that creates current.<ref name="RE2">PV Education. (September 26, 2015). ''Band Gap'' [Online]. Available: http://www.pveducation.org/pvcdrom/pn-junction/band-gap</ref> A small amount of [[doping]] material can drastically increase the conductivity of this material.		In conductors, the valence band overlaps with the conduction band. This overlap causes the valence electrons to essentially be free to move into the conduction band and participate in conduction. Since it is not a full overlap, only a fraction of the valence electrons can move through the material, but this is still enough to make conductors conductive.<ref>HyperPhysics. (September 26, 2015). ''Conductor Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c6</ref>

			In semiconductors, the gap is small enough that it can be bridged by some sort of excitation, perhaps from the [[Sun]] in the case of [[photovoltaic cell]]s (thermal energy can get a small number of electrons across the gap too, but solar cells are engineered for sunlight to drive most of the jumps). The gap is essentially some size "in-between" that of a conductor or insulator. In this model, a finite number of electrons are able to reach the conduction band and conduct small amounts of electricity.<ref>HyperPhysics. (September 26, 2015). ''Semiconductor Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c5</ref> The excitation of this electron also allows additional conduction processes to occur as a result of the [[electron hole]] left behind. An electron from an atom close by can occupy this space, creating a chain reaction of holes and electron movement that creates current.<ref name="RE2">PV Education. (September 26, 2015). ''Band Gap'' [Online]. Available: http://www.pveducation.org/pvcdrom/pn-junction/band-gap</ref> A small amount of [[doping]] material can drastically increase the conductivity of this material.

			== For Further Reading ==

			* [[Valence band]]
			* [[Conduction band]]
			* [[Electron hole]]
			* [[Conductor]]
			* [[Semiconductor]]
			* [[Insulator]]
			* Or explore a [[Special:Random\|random page]]

	==References==		==References==
	{{reflist}}		{{reflist}}[[Category:Uploaded]]

J.williams: 1 revision imported

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Jmdonev at 22:52, 29 September 2015

2015-09-29T22:52:46Z

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[[Category:Done 2015-10-15]]
<onlyinclude>A '''band gap''' is the distance between the [[valence band]] of [[electron]]s and the [[conduction band]]. Essentially, the band gap represents the minimum [[energy]] that is required to excite an electron up to a state in the conduction band where it can participate in conduction.</onlyinclude><ref name="RE2"/> The lower energy level is the valence band, and thus if a gap exists between this level and the higher energy conduction band, energy must be input for electrons to become free. The size and existence of this band gap allows one to visualize the difference between [[conductor]]s, [[semiconductor]]s, and [[insulator]]s.<ref name="RE1">HyperPhysics. (September 26, 2015). ''Band Theory of Solids'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html </ref> These distances can be seen in diagrams known as ''band diagrams'', shown in Figure 1 below.

[[File:2000px-Band_gap_comparison.svg.png|780px|thumb|center|Figure 1. A band gap diagram showing the different sizes of band gaps for conductors, semiconductors, and insulators.<ref>Wikimedia Commons. (September 26, 2015). ''Band Gap Comparison'' [Online]. Available: https://upload.wikimedia.org/wikipedia/commons/thumb/0/0b/Band_gap_comparison.svg/2000px-Band_gap_comparison.svg.png</ref>]]

==Band Gap Sizes==
Figure 1 above illustrates the difference in size of the band gap for insulators, conductors, and semiconductors. The size of this band gap gives the materials some of their distinct properties. In insulators, the electrons in the valence band are separated by a large band gap from the conduction band. This means that there is a large "forbidden" gap in energies preventing electrons from the valence band from jumping up into the conduction band and participating in [[conduction]]. This is provides an explanation for why insulators do not conduct [[electricity]] well.<ref>HyperPhysics. (September 26, 2015). ''Insulator Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c4</ref>

In conductors, the valence band overlaps with the conduction band. This overlap causes the valence electrons to be essentially free to move into the conduction band and participate in conduction. Since it is not a full overlap, only a fraction of the valence electrons can move through the material, but this is still enough to make conductors conductive.<ref>HyperPhysics. (September 26, 2015). ''Conductor Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c6</ref>

In semiconductors, the gap is small enough that it can be bridged by some sort of excitation - perhaps from the [[Sun]] in the case of [[photovoltaic cell]]s. The gap is essentially some size "in-between" that of a conductor or insulator. In this model, a finite number of electrons are able to reach the conduction band and conduct small amounts of electricity.<ref>HyperPhysics. (September 26, 2015). ''Semiconductor Energy Bands'' [Online]. Available: http://hyperphysics.phy-astr.gsu.edu/hbase/solids/band.html#c5</ref> The excitation of this electron also allows additional conduction processes to occur as a result of the [[electron hole]] left behind. An electron from an atom close by can occupy this space, creating a chain reaction of holes and electron movement that creates current.<ref name="RE2">PV Education. (September 26, 2015). ''Band Gap'' [Online]. Available: http://www.pveducation.org/pvcdrom/pn-junction/band-gap</ref> A small amount of [[doping]] material can drastically increase the conductivity of this material.

==References==
{{reflist}}