SrZrO 3 formation at the interface of gadolinia-doped ceria (GDC) interlayer and yttria-stabilized zirconia (YSZ) electrolyte is analyzed using high-resolution electron microscopy. SrZrO 3 is dispersed in the inter-diffusion layer on the GDC side from the Ce/Zr border. Zr, which diffuses into the GDC grain, contributes to the formation of SrZrO 3 . The crystallographic relationship among the SrZrO 3 grains and its neighboring GDC grains reveals that SrZrO 3 is formed at the surface, at the grain boundary, and inside the grain, while maintaining a highly matched boundary with the adjacent GDC grain. The matching of the interface boundary is confirmed by the O-lattice theory, according to which the threshold Zr/Ce ratio is 13/34. If Zr/Ce ratio in the GDC grain is higher than the threshold, SrZrO 3 may significantly grow into the grain. The conduction path for the oxygen ion is retained because the GDC grain containing Zr is split into the SrZrO 3 grain and the less-Zr-containing GDC grain. If Zr/Ce ratio is lower than the threshold, SrZrO 3 may be formed but will be limited by the amount of Zr diffusing from the adjacent region. Thus, the morphology of SrZrO 3 is strongly affected by the state of GDC grains in the inter-diffusion layer. Solid oxide fuel cells (SOFCs) represent a promising technology for converting chemical energy of fuel to electricity with high efficiency, and should find many commercial applications. In the recent developments of SOFCs, lanthanum strontium cobaltite ferrite (La,Sr)(Co,Fe)O 3 (LSCF), with mixed ionic-electronic conductivity, is widely used as the cathode material because it offers high electrochemical performance at intermediate temperatures. Since the most common electrolyte material, i.e. yttria-stabilized zirconia (YSZ), tends to react with LSCF to form highly resistive SrZrO 3 , a thin interlayer consisting of doped ceria, such as gadolinia-doped ceria (GDC), is generally introduced between the LSCF cathode and the electrolyte to prevent solid-state reaction. 1-3 Some manufactures have fabricated an interlayer dense enough to suppress Sr diffusion toward the electrolyte side, which is accompanied by no SrZrO 3 formation. 4 In general, however, the interlayer formed on the YSZ electrolyte by printing and high-temperature sintering becomes porous. Therefore, the interlayer cannot completely eliminate SrZrO 3 formation, and the SrZrO 3 is often formed near the ceria/zirconia interface. [5][6][7][8][9][10][11][12][13][14] The amount and distribution of SrZrO 3 formation depends on the heat-treatment temperature of the interlayer. Wankmüller et al. reported the influence of the sintering temperature of GDC interlayer on the morphology of SrZrO 3 formation. 13 When the sintering temperature of GDC interlayer was 1200 • C, heat-treatment of LSCF cathode at 1080 • C produced a detrimental layer of SrZrO 3 entirely covering the YSZ electrolyte surface. When the sintering temperature of GDC interlayer was higher than 1300 • C, the amount of SrZrO 3 formed decreased and the distributio...