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Dependence of electrical conductivity of nanocrystalline silicon on structural properties and the effect of substrate bias
50
Citations
22
References
1987
Year
EngineeringElectrical ConductivitySemiconductor MaterialsThin Film Process TechnologySilicon On InsulatorSemiconductor DeviceSemiconductor NanostructuresSemiconductorsElectronic DevicesNanoelectronicsDark Electrical ConductivityMaterials ScienceElectrical EngineeringCrystalline DefectsSubstrate BiasNanotechnologyNanocrystalline SiliconRoom-temperature Conductivity σRtSemiconductor MaterialSemiconductor Device FabricationElectrical PropertyElectronic MaterialsSurface ScienceApplied PhysicsThin FilmsAmorphous SolidElectrical Insulation
Abstract The dark electrical conductivity of undoped and phosphorus-doped nanocrystalline (nc) and amorphous (a-) thin films of silicon has been studied as a function of substrate bias between Vb∼0 (floating) and −1000 V under conditions in which all other deposition parameters, such as temperature, deposition rate, discharge current and chemical composition of the plasma, were held constant. With increasing bias from Vb∼0 to −100 V, the room-temperature conductivity σRT of undoped nc-Si decreases from ∼10-−4 to about 10−9 Ω−1 cm−1. A further increase in the bias results in the appearance of a second conductance path which could be attributed to grain boundaries. At a bias of V b < −600 V, a mixture of nc- and a-Si phases are formed with σRT showing a rather complex dependence on V b and approaching that of a-Si for V b∼ −1000 V, where no crystalline component is detectable by X-ray diffraction. Phosphorus-doped nc-Si films prepared under the same conditions and with a gas-doping ratio of [PH3]/[H2] = 10−4 exhibit an almost constant conductivity over the whole bias range between 0 and −850 V. An interpretation of these results is suggested.
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