IEEE Transactions on Electron Devices · 1982 · 79 citations · 26 references
Device ModelingElectrical EngineeringEngineeringNanoelectronicsSurface ScienceApplied PhysicsTime-dependent Dielectric BreakdownTransistor ActionSingle Event EffectsSemiconductor Device FabricationSource-drain BreakdownIntegrated CircuitsShort-channel Mos DevicesDrain-source Avalanche BreakdownMicroelectronicsSurface ConductionSemiconductor DeviceVlsi Scaling
In MOS VLSI device scaling, two major limiting mechanisms are the punchthrough and source-drain breakdown. The punchthrough mechanism is generally considered a bulk-dominated effect. Drain-source avalanche breakdown is generally attributed to bipolar transistor action between drain and source, dominated by injection through the neutral substrate region. The present work includes an experimental verification and a qualitative model demonstrating that both punchthrough and drain-source avalanche breakdown limitations are surface and surface-depletion-region dominated mechanisms, respectively. The two mechanisms are treated simultaneously since both involve enhanced injection from the source due to drain-induced source-potential barrier lowering. The experimental verification is done over a wide range of relevant device parameters, channel implant concentration between 5 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">14</sup> -1 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">16</sup> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> for punchthrough and 2 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">15</sup> -5 × 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">16</sup> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-3</sup> for drain-source avalanche breakdown, effective channel length of 1.0-30.0 µm for both mechanisms.
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A numerical model of avalanche breakdown in MOSFET's
T. Toyabe, Ken Yamaguchi, S. Asai et al. · IEEE Transactions on Electron Devices · 1978 · 155 citations