Mechanism of negative-bias-temperature instability
Although negative-bias-temperature instability in metal-oxide-semiconductor integrated circuits has been minimized empirically, the exact mechanism is unknown. We argue in this paper that the mechanism of negative-bias-temperature instability can be modeled by a first-order electrochemical reaction...
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Published in | Journal of applied physics Vol. 69; no. 3; pp. 1712 - 1720 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Woodbury, NY
American Institute of Physics
01.02.1991
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Subjects | |
Online Access | Get full text |
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Summary: | Although negative-bias-temperature instability in metal-oxide-semiconductor integrated circuits has been minimized empirically, the exact mechanism is unknown. We argue in this paper that the mechanism of negative-bias-temperature instability can be modeled by a first-order electrochemical reaction between hydrogenated trivalent silicon, a neutral water-related species located in the oxide near the Si-SiO2 interface, and holes at the silicon surface to form neutral trivalent silicon and a positively charged water-related species. To show that such a reaction describes the phenomenon, we show that (1) water must be present in the oxide near the Si-SiO2 interface, (2) induced interface and oxide-fixed charge densities are equal, (3) the saturation interface-trap and oxide-fixed charge densities depend on the initial hole concentration at the silicon surface or aging field, (4) the buildup of these charge densities follows first-order reaction kinetics, and (5) time constants for this charge buildup are independent of aging field. The measurements which are done to demonstrate these features combine room-temperature charge measurement using the Q-C method with current measurements during accelerated aging. |
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ISSN: | 0021-8979 1089-7550 |
DOI: | 10.1063/1.347217 |