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{{Use dmy dates|date=
{{short description|Effect in field effect transistors}}
[[File:Mosfet saturation.svg|thumbnail|Cross section of a MOSFET operating in the saturation region]]
To understand the effect, first the notion of '''pinch-off''' of the channel is introduced. The channel is formed by attraction of carriers to the gate, and the current drawn through the channel is nearly a constant independent of drain voltage in saturation mode. However, near the drain, the gate ''and drain'' '''jointly''' determine the electric field pattern. Instead of flowing in a channel, beyond the pinch-off point the carriers flow in a subsurface pattern made possible because the drain and the gate both control the current. In the figure at the right, the channel is indicated by a dashed line and becomes weaker as the drain is approached, leaving a gap of uninverted silicon between the end of the formed inversion layer and the drain (the ''pinch-off'' region).
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In the weak inversion region, the influence of the drain analogous to channel-length modulation leads to poorer device turn off behavior known as [[DIBL|drain-induced barrier lowering]], a drain induced lowering of threshold voltage.
In [[Bipolar junction transistor|bipolar devices]], a similar increase in current is seen with increased collector voltage due to base-narrowing, known as the [[Early effect]]. The similarity in effect upon the current has led to use of the term "Early effect" for MOSFETs as well, as an alternative name for "channel-length modulation".
==Shichman–Hodges model {{anchor|Shichman-Hodges model|Shichman–Hodges model|Shichman-Hodges|Shichman–Hodges}}==
In textbooks, channel length modulation in [[MOSFET#Modes of operation|active mode]] usually is described using the Shichman–Hodges model, accurate only for old technology:<ref>
where <math>
technology parameter sometimes called the transconductance coefficient, ''W
In the classic Shichman–Hodges model, <math>V_\text{th}</math> is a device constant, which reflects the reality of transistors with long channels.
==Output resistance==
Channel-length modulation is important because it decides the MOSFET [[output resistance]], an important parameter in circuit design of [[current mirror]]s and [[amplifiers]].
In the Shichman–Hodges model used above, output resistance is given as:
::<math display="block">\begin{align}
r_\text{O} &= \frac{1 + \lambda V_\text{DS}}{\lambda I_\text{D}} \\
&= \frac{1}{I_\text{D}}\left(\frac{1}{\lambda} + V_\text{DS}\right) \\
&= \frac{V_\text{E} L/{\Delta L} + V_\text{DS}}{I_\text{D}}
\end{align}</math>
where <math>V_\text{DS}</math> = drain-to-source voltage, <math>
| author=W. M. C. Sansen▼
| title=Analog Design Essentials▼
▲|author=W. M. C. Sansen
▲|title=Analog Design Essentials
| publisher=Springer▼
▲|year= 2006
| ___location=Dordrecht▼
▲|publisher=Springer
| isbn=0-387-25746-2▼
▲|___location=Dordrecht
| url=http://worldcat.org/isbn/0387257462▼
▲|isbn=0-387-25746-2
▲|url=http://worldcat.org/isbn/0387257462
| archive-date=22 April 2009
▲|pages=§0124, p. 13}}
| archive-url=https://web.archive.org/web/20090422023023/http://www.worldcat.org/isbn/0387257462
</ref>▼
| url-status=live
▲ }}</ref>
::<math>\lambda
where ''V''<sub>E</sub>
{{Cite book
|
|year= 2003▼
|page=212▼
▲|year= 2003
|publisher=Wiley▼
▲|page=212
|___location=New York▼
▲|publisher=Wiley
|isbn=0-471-49869-6▼
▲|___location=New York
|url=https://books.google.com/books?id=aMUBiiFJYtQC&pg=PA212
▲|isbn=0-471-49869-6
}}</ref>). However, no simple formula used for λ to date provides accurate length or voltage dependence of ''r<sub>O</sub>'' for modern devices, forcing use of computer models, as discussed briefly next.▼
▲</ref>). However, no simple formula used for λ to date provides accurate length or voltage dependence of ''r<sub>O</sub>'' for modern devices, forcing use of computer models, as discussed briefly next.
The effect of channel-length modulation upon the MOSFET output resistance varies both with the device, particularly its channel length, and with the applied bias. The main factor affecting the output resistance in longer MOSFETs is channel length modulation as just described. In shorter MOSFETs additional factors arise such as: [[DIBL|drain-induced barrier lowering]] (which lowers the threshold voltage, increasing the current and decreasing the output resistance), [[velocity saturation]] (which tends to limit the increase in channel current with drain voltage, thereby increasing the output resistance) and [[ballistic transport]] (which modifies the collection of current by the drain, and modifies [[DIBL|drain-induced barrier lowering]] so as to increase supply of carriers to the pinch-off region, increasing the current and decreasing the output resistance). Again, accurate results require [[SPICE#Device models|computer models]].
==References and notes==▼
<references/>▼
==See also==
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*[[Short channel effect]]
*[[DIBL|Drain-induced barrier lowering]]
*[[MOSFET#
*[[Hybrid-pi model]]
*[[Transistor models]]
▲==References and notes==
▲<references/>
==External links==
* [http://www.onmyphd.com/?p=channel.length.modulation What is channel length modulation?] - OnMyPhD
* [http://www.allaboutcircuits.com/technical-articles/mosfet-channel-length-modulation/ MOSFET Channel-Length Modulation] - Tech brief
{{DEFAULTSORT:Channel Length Modulation}}
[[Category:Electronic design]]
[[Category:MOSFETs]]
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