posted on 2016-10-19, 13:33authored byYan Suffren, Olivier Leynaud, Philippe Plaindoux, Alain Brenier, Isabelle Gautier-Luneau
The Ln(IO3)3(HIO3)y (y = 1 or 1.33) compounds are isostructural with the La(IO3)3(HIO3)y phases, but thermal studies reveal different behaviors. On the one
hand, the partial thermal decompositions of these lanthanide compounds
lead to the Ln(IO3)3 formulation, with a room
temperature structure different from the β-La(IO3)3 obtained from La(IO3)3(HIO3)y. On the other hand, the partial
thermal decompositions of the La1–xLnx(IO3)3(HIO3)y compounds prepared with lanthanides
ions (Ce, Pr, Nd, Sm, Eu, Gd, and Yb) lead to acentric β-La1–xLnx(IO3)3. As for β-La(IO3)3, reversible structural transitions from β-La1–xLnx(IO3)3 to centrosymmetric γ-La1–xLnx(IO3)3 are observed. Differential scanning calorimetry analyses of La1–xLnx(IO3)3 solid solutions show that the transition temperatures
vary with the lanthanide concentration in the solid solution. A transition
is observed only up to a certain fraction of lanthanide-ion substitution;
this substitution limit decreases with the cationic radius of the
lanthanide ion. Finally, the β-La1–xNdx(IO3)3 and β-La1–xYbx(IO3)3 phases are investigated
by luminescence spectroscopy.