Applied Physics Letters · 2012 · 74 citations · 13 references
EngineeringElectrical EngineeringPhysicsMicroelectronicsSemiconductor DevicesSemiconductor MaterialsElectrical ConductivityElectronic Transport ModelingMetal-semiconductor ContactsSemiconductor Device MaterialsSemiconductor InterfacesSemiconductor PhysicsConduction BandContact ResistanceElectronic ConductionMetal-induced Gap StatesMetal-semiconductor InterfacesOhmic ConductionOhmic ContactsResistivity
A comprehensive, physics-based unified model is developed for study of low resistivity metal-insulator-semiconductor (M-I-S) ohmic contact. Reduction in metal-induced gap state density and Fermi unpinning in semiconductor as a function of insulator thickness is coupled with electron transport including tunnel resistance through the metal-insulator-semiconductor (M-I-S) system to calculate specific contact resistivity at each insulator thickness for n-Si, n-Ge, and n-InGaAs. Low conduction band offset results in ∼1×10−9 Ω−cm2 contact resistivity with TiO2 insulator on n-Si, ∼7×10−9 Ω−cm2 can be achieved using TiO2 and ZnO on n-Ge, and ∼6×10−9 Ω−cm2 can be achieved with CdO insulator on n-InGaAs, which meet the sub-22nm CMOS requirements.
13
On the physics of metal-semiconductor interfaces
Winfried Mönch · Reports on Progress in Physics · 1990 · 288 citations
Masaharu Kobayashi, Atsuhiro Kinoshita, Krishna C. Saraswat et al. · Journal of Applied Physics · 2009 · 208 citations