Solid oxide fuel cells (SOFCs) are a major candidate technology for clean energy conversion because of their high efficiency and fuel flexibility.[1] The development of intermediate-temperature (500-750 8C) SOFCs requires electrolytes with high oxide ion conductivity (exceeding 10 À2 S cm À1 assuming an electrolyte thickness of 15 mm [1] ). This conductivity, in turn, necessitates enhanced understanding of the mechanisms of oxide ion charge carrier creation and mobility at an atomic level. The charge carriers are most commonly oxygen vacancies in fluorites [2,3] and perovskites. [3,4] There are fewer examples of interstitial-oxygenbased conductors such as the apatites [5,6] and La 2 Mo 2 O 9 -based materials, [7][8][9] so information on how these excess anion defects are accommodated and the factors controlling their mobility is important.The A 2 B 3 O 7 melilite structure consists of anionic layers of five-membered rings of two totally condensed (four neighboring tetrahedra linked by B-O-B bonds) and three partially condensed (three neighboring tetrahedra) BO 4 tetrahedra, separated by sheets of A cations located above the five-ring centers (Figure 1 a, and Figure S1.1 in the Supporting Information). Previously, [10] we demonstrated that A-site substitution in melilite LaSrGa 3 O 7 (A 2 = LaSr, B = Ga) affords La 1.54 Sr 0.46 Ga 3 O 7.27 , in which interstitial oxygen atoms (O int ) are located in the five-rings of the two-dimensional tetrahedral network, gives pure oxide ion conductivity of 0.02-0.1 S cm À1 over the 600-900 8C temperature range.[11] LaCaGa 3 O 7 also adopts the tetragonal melilite structure (space group P4 2 1 m) found for the Sr phase. [12,13] When doped to introduce oxide charge carriers in the La 1+x Ca 1Àx Ga 3 O 7+0.5x series, the tetragonal structure is retained to x = 0.5. Herein, we address the impact on the physical properties of a new lower-symmetry phase formed to accommodate the higher interstitial doping levels 0.55 x 0.64.X-ray powder diffraction from La 1.64 Ca 0.36 Ga 3 O 7.32 (Section 2 in the Supporting Information) indicates that the lowering of symmetry at high doping levels occurs by