Mn and/or rare earth-doped xCaTiO\u2083 - (1-x)CaMeO\u2083 dielectrics, where Me=Hf or Zr and x=0.7, 0.8, and 0.9 were developed to yield materials with room temperature relative permittivities of \u0395 r ~ 150-170, thermal coefficients of capacitance (TCC) of \u00b1 15.8% to \u00b1 16.4% from -50 to 150°C, and band gaps of ~ 3.3-3.6 eV as determined by UV-Vis spectroscopy. Un-doped single layer capacitors exhibited room temperature energy densities as large as 9.0 J/cm\u2083, but showed a drastic decrease in energy density above 100°C. When doped with 0.5 mol% Mn, the temperature dependence of the breakdown strength was minimized, and energy densities similar to room temperature values (9.5 J/cm\u2083) were observed up to 200°C. At 300°C, energy densities as large as 6.5 J/cm\u2083 were measured. These observations suggest that with further reductions in grain size and dielectric layer thickness, the xCaTiO\u2083 - (1-x)CaMeO\u2083 system is a strong candidate for integration into future power electronics applications. To further improve the high temperature, high field reliability of these material systems, rare earth donor doping has been utilized. Initially, 1 mol% doping with Dy, Gd, and Sm showed the most significant reduction in high temperature, high field conductivity. Further investigation of Dy co-doping with 0.5 mol% Mn , Mg, and (Mn+Mg) showed the most significant increase in Ca(Ti\u2080.\u2088Hf
\u2080.\u2082)O\u208
3 resistivity from 4.61 M\u03a9.m with only Mn doping to 176 G\u03a9.cm with Dy and Mg co-doping. Material systems were characterized using capacitance and dielectric loss versus temperature, current-voltage (I-V), UV-Vis spectroscopy for band gap determination, and polarization versus field measurements.
Mn and/or rare earth-doped xCaTiO\u2083 - (1-x)CaMeO\u2083 dielectrics, where Me=Hf or Zr and x=0.7, 0.8, and 0.9 were developed to yield materials with room temperature relative permittivities of \u0395 r ~ 150-170, thermal coefficients of capacitance (TCC) of \u00b1 15.8% to \u00b1 16.4% from -50 to 150°C, and band gaps of ~ 3.3-3.6 eV as determined by UV-Vis spectroscopy. Un-doped single layer capacitors exhibited room temperature energy densities as large as 9.0 J/cm\u2083, but showed a drastic decrease in energy density above 100°C. When doped with 0.5 mol% Mn, the temperature dependence of the breakdown strength was minimized, and energy densities similar to room temperature values (9.5 J/cm\u2083) were observed up to 200°C. At 300°C, energy densities as large as 6.5 J/cm\u2083 were measured. These observations suggest that with further reductions in grain size and dielectric layer thickness, the xCaTiO\u2083 - (1-x)CaMeO\u2083 system is a strong candidate for integration into future power electronics applications. To further improve the high temperature, high field reliability of these material systems, rare earth donor doping has been utilized. Initially, 1 mol% doping with Dy, Gd, and Sm showed the most significant reduction in high temperature, high field conductivity. Further investigation of Dy co-doping with 0.5 mol% Mn , Mg, and (Mn+Mg) showed the most significant increase in Ca(Ti\u2080.\u2088Hf\u2080.\u2082)O\u2083 resistivity from 4.61 M\u03a9.m with only Mn doping to 176 G\u03a9.cm with Dy and Mg co-doping. Material systems were characterized using capacitance and dielectric loss versus temperature, current-voltage (I-V), UV-Vis spectroscopy for band gap determination, and polarization versus field measurements.
