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Floating body effect



The floating body effect is the effect of dependence of the body potential of a transistor realized by the silicon on insulator technology on the history of its biasing and the carrier recombination processes. The transistor's body forms a capacitor against the insulated substrate. The charge accumulates on this capacitor and may cause adverse effects, for example, opening of parasitic transistors in the structure and causing off-state leakages, resulting in higher current consumption and in case of DRAM in loss of information from the memory cells. It also causes the history effect, the dependence of the threshold voltage of the transistor on its previous states. [1]. On analog devices, the floating body effect is known as the kink effect.

One countermeasure to floating body effect involves use of fully depleted devices. The insulator layer in FD devices is significantly thinner than the channel depletion width. The charge and thus also the body potential of the transistors is therefore fixed. [2] However, the short-channel effect is worsened in the FD devices, the body may still charge up if both source and drain are high, and the architecture is unsuitable for some analog devices that require contact with the body. [3]

Hybrid trench isolation is another approach. [4]

While floating body effect presents a problem in SOI DRAM chips, it is exploited as the underlying principle for ZRAM and TTRAM technologies.

References

  1. ^ Berkeley University paper
  2. ^ IBM research
  3. ^ EETimes report
  4. ^ EETimes report
 
This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Floating_body_effect". A list of authors is available in Wikipedia.
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