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RESEARCH PRODUCT

Superior energy density through tailored dopant strategies in multilayer ceramic capacitors

Huijing YangHongfen JiZhilun LuZhilun LuDerek C. SinclairShi-yu LiuLinhao LiGe WangIan M. ReaneyJinglei LiDawei WangAntonio Andre Quadros Da Cunha FeteiraDejun LiWeichao BaoFangfang XuAli MostaedAli Mostaed

subject

Materials scienceDopantRenewable Energy Sustainability and the Environment02 engineering and technologyDielectric010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesPollution0104 chemical scienceslaw.inventionCapacitorNuclear Energy and EngineeringElectrical resistivity and conductivitylawvisual_artvisual_art.visual_art_mediumEnvironmental ChemistryCeramicComposite material0210 nano-technologyCeramic capacitorShort circuitElectrical conductor

description

The Gerson–Marshall (1959) relationship predicts an increase in dielectric breakdown strength (BDS) and therefore, recoverable energy density (Wrec) with decreasing dielectric layer thickness. This relationship only operates however, if the total resistivity of the dielectric is sufficiently high and the electrical microstructure is homogeneous (no short circuit diffusion paths). BiFeO3–SrTiO3 (BF–ST) is a promising base for developing high energy density capacitors but Bi-rich compositions which have the highest polarisability per unit volume are ferroelectric rather than relaxor and are electrically too conductive. Here, we present a systematic strategy to optimise BDS and maximum polarisation via: (i) Nb-doping to increase resistivity by eliminating hole conduction and promoting electrical homogeneity and (ii) alloying with a third perovskite end-member, BiMg2/3Nb1/3O3 (BMN), to reduce long range polar coupling without decreasing the average ionic polarisability. These strategies result in an increase in BDS to give Wrec = 8.2 J cm−3 at 460 kV cm−1 for BF–ST–0.03Nb–0.1BMN ceramics, which when incorporated in a multilayer capacitor with dielectric layers of 8 μm thickness gives BDS > 1000 kV cm−1 and Wrec = 15.8 J cm−3.