JpGU-AGU Joint Meeting 2020

講演情報

[E] ポスター発表

セッション記号 S (固体地球科学) » S-MP 岩石学・鉱物学

[S-MP36] 鉱物の物理化学

コンビーナ:鎌田 誠司(東北大学学際科学フロンティア研究所)、鹿山 雅裕(東京大学大学院総合文化研究科広域科学専攻広域システム科学系)

[SMP36-P05] Density and elastic properties of liquid gallium using externally heated diamond anvil cell

*鶴岡 椋1寺崎 英紀1鎌田 誠司2,3前田 郁也3近藤 忠1山田 伊織1浦川 啓4米田 明5平尾 直久6河口 沙織6町田 晃彦7 (1.大阪大学大学院理学研究科宇宙地球科学専攻、2.東北大学学際科学フロンティア研究所、3.東北大学大学院理学研究科地学専攻、4.岡山大学大学院自然科学研究科、5.岡山大学惑星物質研究所、6.高輝度光科学研究センター、7.量子科学技術研究開発機構)

キーワード:ガリウム、ダイアモンドアンビルセル、X線吸収法

It is important to measure density of liquid metals at high pressure and high temperature for understanding compression behavior and elastic properties of liquid metals. Since gallium (Ga) has a low melting temperature, Ga can become liquid state easily under high pressure. The densities of liquid Ga have been reported by X-ray tomography (Li et al. 2014), by sound velocity (Ayrinhac et al. 2015), by reverse Monte Carlo simulations combined with X-ray scattering data (Yu et al. 2012). However these densities were not consistent with each other. X-ray absorption method is effective to measure liquid density directly. In this study, the densities of liquid gallium were measured using X-ray absorption method combined with an externally heated diamond anvil cell (DAC).

In X-ray absorption method, density of liquid Ga was obtained from measured incident and transmitted X-ray intensities of the samples using Lambert-Beer law (Takubo et al. 2019). Ga sample and two reference materials (RbBr, KBr, or Fe) were loaded into each hole drilled on a pre-indented Re gasket. The Re gasket was coated with Al2O3 to avoid a reaction between the Ga sample and the gasket. High pressure was generated using a symmetric DAC with a lever-arm frame. High temperature was generated using external heaters composed of Pt-Rh wires with a ZrO2 insulator. X-ray absorption measurements were conducted with monochromatic X-ray of 30 keV at BL10XU and BL22XU beamlines in SPring-8.

The density of liquid Ga were measured up to 10 GPa and 533 K. The elastic properties (bulk modulus (KT0), its pressure derivative (K')) of liquid Ga were calculated by fitting the density data with equations of state (EOSs) and obtained 45.8(4) GPa, 6.1(2) from third-order Birch-Murnaghan EOS at 500 K, respectively. In lower pressure region, the compression curve is consistent with the density calculated from sound velocity data reported by Ayrinhac et al. (2015). However, our results show that density variation is smaller than Ayrinhac et al. (2015) in higher pressure (e.g. 1% smaller at 10 GPa).