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Materials Data on YbO2 by Materials Project

YbO2 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Yb is bonded to six equivalent O atoms to form a mixture of distorted edge and corner-sharing YbO6 octahedra. The corner-sharing octahedral tilt angles are 72°. There are two shorter (2.16 Å) and four longer (2.35 Å) Yb–O bond lengths. O is bonded in a 1-coordinate geometry to three equivalent Yb and one O atom. The O–O bond length is 1.46 Å.

36 MATERIALS SCIENCE↗

Materials Data on YbO2 by Materials Project

YbO2 is Baddeleyite-like structured and crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are three inequivalent Yb sites. In the first Yb site, Yb is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Yb–O bond distances ranging from 2.30–2.36 Å. In the second Yb site, Yb is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Yb–O bond distances ranging from 2.30–2.35 Å. In the third Yb site, Yb is bonded in a 7-coordinate geometry to seven O atoms. There are a spread of Yb–O bond distances ranging from 2.31–2.35 Å. There are six inequivalent O sites. In the first O site, O is bonded to four Yb atoms to form a mixture of corner and edge-sharing OYb4 tetrahedra. In the second O site, O is bonded to four Yb atoms to form a mixture of corner and edge-sharing OYb4 tetrahedra. In the third O site, O is bonded to four Yb atoms to form a mixture of corner and edge-sharing OYb4 tetrahedra. In the fourth O site, O is bonded in a distorted trigonal planar geometry to three Yb atoms. In the fifth O site, O is bonded in a distorted trigonal planar geometry to three Yb atoms. In the sixth O site, O is bonded in a distorted trigonal planar geometry to three Yb atoms.

36 MATERIALS SCIENCE↗

Alumina Paste Layer as a Sublimation Suppression Barrier for Yb14MnSb11

Sublimation is a major cause of degradation of thermoelectric power generation systems. Most thermoelectric materials tend to have peak values at the temperature where sublimation occurs. A sublimation barrier is needed that is stable at operating temperatures, inert against thermoelectric materials, and able to withstand thermal cycling stress. A porous alumina paste layer is suitable as a sublimation barrier for Yb14MnSb11. It can accommodate stress generated by the thermal expansion discrepancy between the suppression layer and thermoelectric materials. Sublimation suppression is achieved by filling pores naturally with YbO2, a natural byproduct of sublimation. YbO2 generated during the sublimation of Yb14MnSb11 fills the porous structure of the alumina paste, causing sublimation to decrease with time as the pores become filled.

Paik, Jong-Ah↗