Skull Melting Growth and Characterization of (ZrO<sub>2</sub>)<sub>0.89</sub>(Sc<sub>2</sub>O<sub>3</sub>)<sub>0.1</sub>(CeO<sub>2</sub>)<sub>0.01</sub> Crystals
Dmitrii Agarkov,
Mikhail Borik,
Galina Eliseeva,
Alexey Kulebyakin,
Elena Lomonova,
Filipp Milovich,
Valentina Myzina,
Yuriy Parkhomenko,
Elena Skryleva,
Nataliya Tabachkova
Affiliations
Dmitrii Agarkov
Institute of Solid State Physics, Russian Academy of Sciences, Academician Osip’yan str. 2, Chernogolovka, 142432 Moscow, Russia
Mikhail Borik
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
Galina Eliseeva
Institute of Solid State Physics, Russian Academy of Sciences, Academician Osip’yan str. 2, Chernogolovka, 142432 Moscow, Russia
Alexey Kulebyakin
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
Elena Lomonova
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
Filipp Milovich
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
Valentina Myzina
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
Yuriy Parkhomenko
National University of Science and Technology (MISIS), Leninskiy prospekt 4, 119049 Moscow, Russia
Elena Skryleva
National University of Science and Technology (MISIS), Leninskiy prospekt 4, 119049 Moscow, Russia
Nataliya Tabachkova
Prokhorov General Physics Institute, Russian Academy of Sciences, VavilovStr. 38, 119991 Moscow, Russia
(ZrO2)0.89(Sc2O3)0.1(CeO2)0.01 crystals have been grown by directional melt crystallization in a cold crucible. The chemical and phase compositions of the crystals have been characterized using energy dispersion X-ray spectroscopy (EDX), Raman scattering spectroscopy and transmission electron microscopy (TEM). The X-ray photoelectron emission method has been used for determining the valence state of the Ce ions. We show that directional melt crystallization produces an inhomogeneous ceria distribution along the crystal length. The as-grown crystals are mixtures of cubic and rhombohedral zirconia modifications. The rhombohedral phase has an inhomogeneous distribution along crystal length. Melt crystallization does not produce single-phase cubic (ZrO2)0.89(Sc2O3)0.1(CeO2)0.01 crystals. The formation of the phase structure in the crystals for different synthesis methods has been discussed.