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Reliability constraints for TANOS memories due to alumina trapping and leakage
13
Citations
8
References
2010
Year
Unknown Venue
Non-volatile MemoryEngineeringEmerging Memory TechnologyComputer ArchitectureTanos MemoriesMemory DeviceElectronic PackagingReliability ConstraintsMaterials EngineeringElectrical EngineeringHardware ReliabilityElectronic MemoryComputer EngineeringThreshold InstabilityTanos Memory ReliabilityMicroelectronicsApplied PhysicsSemiconductor MemoryTanos Devices
In this work we present a detailed investigation of TANOS memory reliability, focusing on issues raised by Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> trapping/detrapping and leakage. These effects are investigated as a function of alumina thickness, electric field and temperature, comparing experimental and modeling results for trap parameters extraction. For TANOS devices, Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> charge storage modifies program and erase saturation level particularly when higher Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> thikness are considered. Threshold instability in early steps for endurance and retarded behavior for retention can be also ascribed to the Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> trapping. Moreover, Al <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</sub> layer has been shown to provide the main leakage path for bottom oxides thickness in the 4.5 nm or above range.
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