The chloride ion is well known as one of several migrating anion species in the solid electrolyte field. However, the chloride-ion conductors reported so far are all based on chlorides that are soluble in hot water or water at room temperature. This can be a critical disadvantage for the practical applications of various functional materials. In order to overcome this problem, it is essential to fabricate Cl À ionconducting solid electrolytes that are water-insoluble. Since the desired end material is a Cl À ion-conductor, the solids should contain Cl À anions. We have previously reported the Ca-doped lanthanum oxychloride solid-solution electrolyte, [1] which has the unique characteristic of being water-insoluble. However, the Cl À ion conductivity at 700 8C was 2.8 î 10 À5 S cm À1 , which is still two orders of magnitude lower than conventional Cl À -ion conductors such as PbCl 2 , [2] BaCl 2 , [3] SrCl 2 , [4] and CsPbCl 3 . [5] This report centers on how the properties of this promising material were improved through a ball milling process. Ball milling resulted in a fine, homogeneous mixture of the starting materials, namely LaOCl and CaCO 3 , which in turn enabled the fabrication of high-density pellets. Figure 1 shows the powder X-ray diffraction (XRD) results for La 1Àx Ca x OCl 1Àx (x ¼ 0.05±0.4) solid solutions, along with the data for pure LaOCl. It is expected that LaOCl would form a solid solution with CaCO 3 with up to 20 mol % CaCO 3 . Since the radii of La 3þ ions and Ca 2þ ions are so similar (0.130 [6] and 0.126 nm, [6] respectively), it is not possible to verify the formation of the solid solution based on changes of lattice parameter. A mixed phase consisting of Ca-doped LaOCl solid solution and CaO was obtained by mixing in CaCO 3 at a proportion of above 20 mol %. This clearly indicates that the solubility limit of Ca in LaOCl is around 20 mol %. Figure 2 presents the electrical conductivity of La 1Àx Ca x OCl 1Àx at 800 8C as a function of x. At a dopant level of 5 mol % Ca, a sharp enhancement in conductivity of over three orders of magnitude is observed. The Cl À vacancies formed by substitution of La 3þ ions by Ca 2þ ions greatly facilitates Cl À anion conduction in the LaOCl framework. The conductivity gradually increases with increasing Ca content in the La 1Àx Ca x OCl 1Àx solid solution, with the highest (1.9 î 10 À2 S cm À1 ) observed for La 0.8 Ca 0.2 OCl 0.8 , which corresponds to x ¼ 0.2. A further increase of the Ca content results in a rapid decrease in conductivity, which results from the formation of the secondary CaO phase. These results corroborate that LaOCl forms a La 1Àx Ca x OCl 1Àx solid solution with up to 20 mol % Ca doping. Figure 3 displays the conductivity of La 0.8 Ca 0.2 OCl 0.8 , which exhibits the highest Cl À ion conductivity in the La 1Àx Ca x OCl 1Àx series, as a function of temperature. This is presented with data for pure LaOCl, the previously reported 1.6 mol % Ca-doped LaOCl solid solution, [1] and two typical Cl À conductors, namely PbCl 2 and CsPbCl 3...