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| [[File:Barrier lowering.PNG|thumbnail|300px|As channel length decreases, the barrier ''φ<sub>B</sub>'' to be surmounted by an electron from the source on its way to the drain reduces]]
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| '''Drain-induced barrier lowering''' or '''DIBL''' is a [[short-channel effect]] in [[MOSFET]]s referring originally to a reduction of [[threshold voltage]] of the [[transistor]] at higher drain voltages.
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| In a classic planar [[field-effect transistor]] with a long channel, the bottleneck in channel formation occurs far enough from the drain contact that it is electrostatically shielded from the drain by the combination of the substrate and gate, and so classically the [[threshold voltage]] was independent of drain voltage.
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| In short-channel devices this is no longer true: The drain is close enough to gate the channel, and so a high drain voltage can open the bottleneck and turn on the transistor prematurely.
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| The origin of the threshold decrease can be understood as a consequence of charge neutrality: the Yau charge-sharing model.
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| <ref name=Arora>
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| {{cite book
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| |author=Narain Arora
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| |title=Mosfet Modeling for VLSI Simulation: Theory And Practice
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| |page=197, Fig. 5.14
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| |year= 2007
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| |publisher=World Scientific
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| |isbn=981-256-862-X
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| |url=http://books.google.com/books?id=SkT2xOuvpuYC&pg=PA197&dq=yau+charge-sharing&sig=NQvLlUOMlEsNFn-oL8y31GFI_Is}}
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| </ref> The combined charge in the [[depletion region]] of the device and that in the channel of the device is balanced by three electrode charges: the gate, the source and the drain. As drain voltage is increased, the [[depletion region]] of the [[p-n junction]] between the drain and body increases in size and extends under the gate, so the drain assumes a greater portion of the burden of balancing depletion region charge, leaving a smaller burden for the gate. As a result, the charge present on the gate retains charge balance by attracting more carriers into the channel, an effect equivalent to lowering the threshold voltage of the device.
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| In effect, the channel becomes more attractive for electrons. In other words, the potential energy barrier for electrons in the channel is lowered. Hence the term "barrier lowering" is used to describe these phenomena. Unfortunately, it is not easy to come up with accurate analytical results using the barrier lowering concept.
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| Barrier lowering increases as channel length is reduced, even at zero applied drain bias, because the source and drain form [[pn junction]]s with the body, and so have associated built-in depletion layers associated with them that become significant partners in charge balance at short channel lengths, even with no reverse bias applied to increase [[depletion width]]s.
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| The term DIBL has expanded beyond the notion of simple threshold adjustment, however, and refers to a number of drain-voltage effects upon MOSFET ''I-V'' curves that go beyond description in terms of simple threshold voltage changes, as described below.
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| As channel length is reduced, the effects of DIBL in the [[subthreshold region]] (weak inversion) show up initially as a simple translation of the subthreshold current vs. gate bias curve with change in drain-voltage, which can be modeled as a simple change in threshold voltage with drain bias. However, at shorter lengths the slope of the current vs. gate bias curve is reduced, that is, it requires a larger change in gate bias to effect the same change in drain current. At extremely short lengths, the gate entirely fails to turn the device off. These effects cannot be modeled as a threshold adjustment.<ref name=Tsividis>
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| {{cite book
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| |author=Yannis Tsividis
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| |title=Operational Modeling of the MOS Transistor
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| |page=268; Fig. 6.11
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| |year= 1999
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| |edition=Second Edition
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| |publisher=McGraw-Hill
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| |location=New York
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| |isbn=0-07-065523-5
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| |url=http://worldcat.org/isbn/0070655235}}
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| </ref>
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| DIBL also affects the current vs. drain bias curve in the [[MOSFET#Modes of operation|active mode]], causing the current to increase with drain bias, lowering the MOSFET output resistance. This increase is additional to the normal [[channel length modulation]] effect on output resistance, and cannot always be modeled as a threshold adjustment.
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| In practice, the DIBL can be calculated as follows:
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| :: <math> \mathrm{DIBL} = - \frac{V_{Th}^{DD} - V_{Th}^{\mathrm{low}}}{V_{DD} - V_{D}^{\mathrm{low}}}, </math>
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| where <math>V_{Th}^{DD}</math> is the threshold voltage measured at a supply voltage (the high drain voltage), and <math>V_{Th}^{\mathrm{low}}</math> is the threshold voltage measured at a very low drain voltage, typically 0.05 V or 0.1 V. <math>V_{DD}</math> is the supply voltage (the high drain voltage) and <math>V_{D}^{\mathrm{low}}</math> is the low drain voltage (for a linear part of device I-V characteristics). The minus in the front of the formula ensures a positive DIBL value. This is because the high drain threshold voltage, <math>V_{Th}^{DD}</math>, is always smaller than the low drain threshold voltage, <math>V_{Th}^{\mathrm{low}}</math>. Typical units of DIBL are mV/V.
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| DIBL can reduce the device operating frequency as well, as described by the following equation:
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| :: <math>\frac{\Delta f}{f} = -\frac{2 \mathrm{DIBL}}{V_{DD}-V_{Th}},</math>
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| where <math>V_{DD}</math> is the supply voltage and <math>V_{Th}</math> is the threshold voltage.
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| ==References==
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| <references/>
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| ==See also==
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| *[[Channel length modulation]]
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| *[[Threshold voltage]]
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| *[[MOSFET#MOSFET structure and channel formation|MOSFET operation]]
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| [[Category:Transistor modeling]]
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Corporate Basic Manager Falkenstein from Dartmouth, likes to spend time quilting, como ganhar dinheiro na internet and hot air balooning. Gets immense motivation from life by likely to locales for example Hatra.