Crystal Structure and Electrical Properties of Ruthenium-Substituted Calcium Copper Titanate

This paper reports a detailed study of crystal structure and dielectric properties of ruthenium-substituted calcium-copper titanates (CaCu(3)Ti(4−x)Ru(x)O(12), CCTRO). A series of three samples with different stoichiometry was prepared: CaCu(3)Ti(4−x)Ru(x)O(12), x = 0, 1 and 4, abbreviated as CCTO, CCT3RO and CCRO, respectively. A detailed structural analysis of CCTRO samples was done by the Rietveld refinement of XRPD data. The results show that, regardless of whether Ti(4+) or Ru(4+) ions are placed in B crystallographic position in AA’(3)B(4)O(12) (CaCu(3)Ti(4−x)Ru(x)O(12)) unit cell, the crystal structure remains cubic with [Formula: see text] symmetry. Slight increases in the unit cell parameters, cell volume and interatomic distances indicate that Ru(4+) ions with larger ionic radii (0.62 Å) than Ti(4+) (0.605 Å) are incorporated in the CaCu(3)Ti(4−x)Ru(x)O(12) crystal lattice. The structural investigations were confirmed using TEM, HRTEM and ADF/STEM analyses, including EDXS elemental mapping. The effect of Ru atoms share in CaCu(3)Ti(4−x)Ru(x)O(12) samples on their electrical properties was determined by impedance and dielectric measurements. Results of dielectric measurements indicate that one atom of ruthenium per CaCu(3)Ti(4−x)Ru(x)O(12) unit cell transforms dielectric CCTO into conductive CCT3RO while preserving cubic crystal structure. Our findings about CCTO and CCT3RO ceramics promote them as ideal tandem to overcome the problem of stress on dielectric-electrode interfaces in capacitors.