2016 · 12 citations · 10 references
EngineeringElectrical EngineeringPhysicsElectronic MaterialsMicroelectronicsSemiconductor DevicesDevice ModelingGraphene NanomaterialsInterconnect TechnologySemiconductor Device MaterialsSemiconductor PhysicsThin Film Electrical PropertiesCapacitanceCircuit Delay ModelingContact ResistanceHexagonal Boron NitrideInterconnect DelayInterconnect Delay ModelingInterconnect Resistance ModelingPhonon Scattering
We modeled the electrostatic doping in multilayer graphene interconnects by self-consistently solving Poisson's equation and we computed the resistivity per layer by accounting for acoustic and optical phonon scattering. For the analysis, we used two different doping concentrations, representative for graphene on top of hexagonal Boron Nitride and SiO <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> substrates. Finally, we benchmarked graphene against Cu interconnects at 10 nm half-pitch in terms of resistance, capacitance, RC delay and circuit delay. Our results show that at least ten layers of graphene are needed in order to achieve lower resistance than Cu. On the other hand, due to the reduced graphene thickness, only four graphene layers are required to outperform Cu in terms of RC delay, because of the lower capacitance. About circuit delay, depending on the assumed contact resistance value, five to ten graphene layers are needed for 3.2 μm long wires to outperform Cu at the 5 nm logic technology node.
10
First-principles analysis of electron-phonon interactions in graphene
K. M. Borysenko, Jeffrey T. Mullen, Edwin Barry et al. · Physical Review B · 2010 · 227 citations · Full text