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Implication of Channel Percolation in Ferroelectric FETs for Threshold Voltage Shift Modeling
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2020
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Device ModelingHafnia-based FefetsElectrical EngineeringEngineeringPhysicsGate Bias DependenceFerroelectric ApplicationChannel PercolationFerroelectric FetsApplied PhysicsCondensed Matter PhysicsThreshold VoltageBias Temperature InstabilityMicroelectronicsSemiconductor Device
Unraveling the gate bias dependence of threshold voltage (V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> ) shift in hafnia-based FeFETs is a central element to device design and reliable operation. Here we present a domain-percolation-based ferroelectric (FE) V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> shift model, in which we attribute the FE-induced V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> lowering to the source-to-drain "clustering" of successively flipped-up FE domains, as the global polarization increases with the gate bias. We highlight our accurate, semi-quantitative modeling reproduction of the experimental V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> shift in our Hf <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</sub> Zr <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.5</sub> O <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> n-FeFET hardware in the presence of traps, where a turnaround of V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> shift versus gate bias is observed. We argue that the turnaround occurs because the FE V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> lowering only starts to prevail when the gate bias has flipped up enough FE domains to "cluster" from source to drain, before which V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">TH</sub> keeps increasing with the gate bias due to charge trapping. The trapping behavior is simulated by a two-state non-radiative multi-phonon model. We further predict that the downscaling of gate length (L <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">g</sub> ) can facilitate the onset of percolation in FE layer, which intrinsically helps to reduce the FE programming voltage (V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">PGM</sub> , by ~0.8V when ideal, trap-free) in FeFETs.