Synthesis, Crystal Structure, and Electronic Properties
of the CaRE<sub>3</sub>SbO<sub>4</sub> and Ca<sub>2</sub>RE<sub>8</sub>Sb<sub>3</sub>O<sub>10</sub> phases (RE = Rare-Earth Metal)
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Abstract
Through
high temperature synthesis at 1300 °C and above, our
group has discovered and characterized the novel CaRE<sub>3</sub>SbO<sub>4</sub> and Ca<sub>2</sub>RE<sub>8</sub>Sb<sub>3</sub>O<sub>10</sub> phases (RE = Ce–Nd, Sm–Dy for CaRE<sub>3</sub>SbO<sub>4</sub>, RE = La–Nd, Sm–Dy for Ca<sub>2</sub>RE<sub>8</sub>Sb<sub>3</sub>O<sub>10</sub>). This result was motivated by
the idea of opening a band gap and introducing structural complexity
in the rare-earth antimonide framework by incorporation of rare-earth
oxide and calcium oxide. The CaRE<sub>3</sub>SbO<sub>4</sub> phases
adopt the tetragonal <i>I</i>4/<i>m</i> symmetry
while the Ca<sub>2</sub>RE<sub>8</sub>Sb<sub>3</sub>O<sub>10</sub> ones adopt the monoclinic <i>C</i>2/<i>m</i> symmetry. These structures show many similarities to the other RE–Sb–O
phases discovered recently, particularly to the RE<sub>3</sub>SbO<sub>3</sub> and RE<sub>8</sub>Sb<sub>3</sub>O<sub>8</sub> phases, in
which a prolonged heat treatment results in one structure converting
to another by elongation of the rare-earth oxide slabs. Electrical
resistivity measurements yielded semiconducting properties for both
series, despite the unbalanced electron count for Ca<sub>2</sub>RE<sub>8</sub>Sb<sub>3</sub>O<sub>10</sub> and electronic structure calculations
that support metallic-type conduction. This unusual behavior is attributed
to Anderson-type localization of Sb p states near the Fermi level,
which arises from the highly disordered Sb layers in the structure.
This Sb disorder was shown to be tunable with respect to the size
of the rare-earth used, improving the electrical resistivity by approximately
1 order of magnitude for each rare-earth in the series