TY - JOUR
T1 - Low-temperature x-ray crystal structure analysis of the cage-structured compounds MBe13 (M=La,Sm, and U)
AU - Hidaka, Hiroyuki
AU - Nagata, Ryoma
AU - Tabata, Chihiro
AU - Shimizu, Yusei
AU - Miura, Naoyuki
AU - Yanagisawa, Tatsuya
AU - Amitsuka, Hiroshi
N1 - Funding Information:
The authors thank Dr. S. Tsutsui for fruitful discussions. The present research was supported by JSPS KAKENHI Grants No. JP20224015(S), No. JP25400346(C), No. JP26400342(C), No. JP15KK0146, No. JP15H05882, and No. JP15H05885 (J-Physics).
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/5/9
Y1 - 2018/5/9
N2 - The beryllides MBe13(M = rare earths and actinides) crystallize in a NaZn13-type cubic structure, which can be categorized as a cage-structured compound. In this study, powder x-ray diffraction measurements have been performed on LaBe13,SmBe13, and UBe13 in the temperature range between 7 and 300 K in order to investigate their crystallographic characteristics systematically. They keep the NaZn13-type cubic structure down to the lowest temperature. We estimated their Debye temperature to be 600-750 K from analyses of the temperature dependence of a lattice parameter, being in good agreement with the values reported previously. Rietveld refinements on the obtained powder patterns revealed that the M atom in the 8a site is located in an almost ideal snub cube formed by 24BeII atoms in the 96i site, whose caged structure is unchanged even at the low temperatures. In addition, it is argued from the temperature variation of an isotropic mean-square displacement parameter that the MBe13 compounds commonly have a low-energy phonon mode, which can be described by a model assuming an Einstein oscillation of the M atom with a characteristic temperature of ∼160 K.
AB - The beryllides MBe13(M = rare earths and actinides) crystallize in a NaZn13-type cubic structure, which can be categorized as a cage-structured compound. In this study, powder x-ray diffraction measurements have been performed on LaBe13,SmBe13, and UBe13 in the temperature range between 7 and 300 K in order to investigate their crystallographic characteristics systematically. They keep the NaZn13-type cubic structure down to the lowest temperature. We estimated their Debye temperature to be 600-750 K from analyses of the temperature dependence of a lattice parameter, being in good agreement with the values reported previously. Rietveld refinements on the obtained powder patterns revealed that the M atom in the 8a site is located in an almost ideal snub cube formed by 24BeII atoms in the 96i site, whose caged structure is unchanged even at the low temperatures. In addition, it is argued from the temperature variation of an isotropic mean-square displacement parameter that the MBe13 compounds commonly have a low-energy phonon mode, which can be described by a model assuming an Einstein oscillation of the M atom with a characteristic temperature of ∼160 K.
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U2 - 10.1103/PhysRevMaterials.2.053603
DO - 10.1103/PhysRevMaterials.2.053603
M3 - Article
AN - SCOPUS:85056591439
SN - 2475-9953
VL - 2
JO - Physical Review Materials
JF - Physical Review Materials
IS - 5
M1 - 053603
ER -