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An ionic compound with the fluorite structure at ordinary conditions.

An ionic compound with the fluorite structure at ordinary conditions.

Eight nearest neighbours at cube corners around a central site; fluorite structure cations have this arrangement.

The conventional cubic cell has volumeConsequently the same effective carrier count isA noninteger mean is normal for a doped crystal: it describes an ensemble average, not a requirement that every cell contain the same number of defects. The fluorite structure has four cation sites and eight oxygen sites in this conventional cell.

The fluorite structure consists of a face-centered cubic lattice of calcium sites with all eight tetrahedral interstitial sites occupied by fluoride. In fractional coordinates of the conventional cubic unit cell, the calcium basis is $(0,0,0),(0,\frac{1}{2},\frac{1}{2}),(\frac{1}{2},0,\frac{1}{2}),(\frac{1}{2},\frac{1}{2},0)$, and fluoride occupies all combinations $(x,y,z)$ with $x,y,z\in \{\frac{1}{4},\frac{3}{4}\}$. The projection therefore superposes two fluoride sites at each quarter-coordinate position. Labels in the original diagram give fractional depth along $[001]$; periodic boundary sites are displayed on both edges.

Counting shared sites gives $8/8+6/2=4$ calcium sites and eight interior fluoride sites: four formula units per conventional cell.

A larger barium cation expands the fluorite structure and can widen the constrictions through which fluoride ions move. A plausible explanation is therefore a smaller ionic migration barrier and greater fluoride mobility. In a simple dilute-carrier description, ${\sigma }_{\mathrm{ion}}=n|q|\mu$, or $n{q}^{2}D/(k_{B}T)$ when an uncorrelated Nernst-Einstein relation applies. fluoride vacancies and interstitial defects, including those generated as Frenkel pairs, provide possible carriers.

More open migration pathways can raise the conductivity, but ion size by itself is not a proof: defect formation free energies set $n$, migration free energies set mobility, and correlated hopping can alter the simple relation. A controlled comparison would use crystals with comparable impurity content, thermal history and electrode conditions, and measure conductivity over temperature to separate plausible activation behaviour from extrinsic defect effects.

The fluorite structure has Ce on the corner and face-centre sites of a face-centered cubic lattice. Oxygen occupies all eight positions $(x,y,z)$ with each coordinate independently $1/4$ or $3/4$. In projection, there are four oxygen positions $(1/4,1/4),(1/4,3/4),(3/4,1/4),(3/4,3/4)$, each representing two heights. Accounting for shared boundary sites gives four Ce and eight O per conventional unit cell.