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NBTI: An Atomic-Scale Defect Perspective
55
Citations
34
References
2006
Year
Unknown Venue
Atomic-scale Defect PerspectiveEngineeringMagnetic ResonanceDefect ToleranceSemiconductor DeviceSemiconductorsSemiconductor TechnologyElectrical EngineeringPhysicsCrystalline DefectsBias Temperature InstabilityAtomic PhysicsDefect FormationSemiconductor Device FabricationDiode Dc-iv MeasurementsMicroelectronicsNbti-induced GenerationBond CenterSpintronicsApplied PhysicsCondensed Matter Physics
We utilize a combination of MOSFET-gate controlled diode DC-IV measurements and a very sensitive electrically-detected electron spin resonance technique called spin-dependent recombination to observe and identify defect centers generated during NBTI in fully processed SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> and plasma nitrided oxide (PNO)-based pMOSFETs. In SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> devices, we observe the NBTI-induced generation of two Si/SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> interface silicon dangling bond centers (P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b0 </sub> and P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b1</sub> ) and very likely an oxide silicon dangling bond center (E'). Our observations indicate that both P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b0</sub> and P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b1</sub> defects play major roles in these SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> -based devices and also suggest that E' centers could play an important role. In PNO devices, we observed the NBTI-induced generation of a new defect center which is fundamentally different from the P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b0</sub> /P <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b1 </sub> defects generated during NBTI in SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> devices. Our results indicate that it plays a dominating role in NBTI-induced interface state generation in thin PNO devices and also exhibits a post-negative bias temperature stress (NBTS) recovery. Although we observe different interface state defects, we observed essentially equivalent activation energies in both the SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> and PNO devices
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