“…While doping at the B-site of Co-based double perovskites (e.g., with Fe, Mn, or Cu) has been relatively thoroughly studied (Karppinen et al, 2002;Zhang, 2004;Tsvetkov et al, 2011;Kim et al, 2013;Broux et al, 2014;Tsvetkov et al, 2016;Kong, 2018;Olszewska and Świerczek, 2019;, in the case of this type of double perovskites, the occupancy of the A-sites can have an equally great impact on the properties of the materials, creating further opportunities for their tailoring. In fact, most of the properties, such as oxygen non-stoichiometry, electronic conductivity, ionic conductivity, or thermal expansion coefficient (TEC), can be directly correlated to the ionic radius of the A-site lanthanide and/or its difference when compared to Ba cations, see also Supplementary Figure S1 (Lee et al, 1998;Du et al, 2014;Kim and Manthiram, 2015;Olszewska, Świerczek, et al, 2019). In most cases, the selection of bigger RE ions, such as La or Pr, helps in enhancing the transport properties, however, at a price of increasingly high TEC values (Kim and Manthiram, 2015) (e.g., from 18.2 to 29.5•10 -6 K −1 for YBaCo 2 O 5+δ and LaBaCo 2 O 5+δ , respectively) (Olszewska, Świerczek, et al, 2019) Similarly, the oxygen nonstoichiometry also changes drastically, varying at room temperature from δ ≈ 0.41 to δ ≈ 1 for Y-and La-based compositions, respectively, and can be further modified by substituting Ba with other smaller alkali ions such as Sr or Ca (Kim and Manthiram, 2015).…”