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$$P$$-$$T$$ phase diagram and structural transformations of molten P$$_{2}$$O$$_{5}$$ under pressure

P$$_{2}$$O$$_{5}$$の圧力温度相図と融体の高圧下の構造変化

Brazhkin, V. V.*; 片山 芳則; Lyapin, A. G.*; 齋藤 寛之

Brazhkin, V. V.*; Katayama, Yoshinori; Lyapin, A. G.*; Saito, Hiroyuki

P$$_{2}$$O$$_{5}$$は典型的なガラス形成酸化物である。我々は、P$$_{2}$$O$$_{5}$$の圧力-温度相図と圧力下での液体P$$_{2}$$O$$_{5}$$の構造変化のX線回折その場観察測定を10GPaまで行った。その結果、圧力下での液体P$$_{2}$$O$$_{5}$$の構造変化は独特な3段階で起こることが明らかになった。すなわち、まず、4GPaまでは、ゆっくりとした平均配位数$$<$$N$$_{1}>$$の増加を伴った中距離秩序の消失が起きる。その後、8-9GPaまでは、構造は変化せず、通常の圧縮が起きる。最後に、9-10GPaで、$$<$$N$$_{1}>$$の急激な増加を伴う急激な短距離秩序の変化が起きる。

The P$$_{2}$$O$$_{5}$$ compound is an archetypical glass-forming oxide. We present the in situ X-ray diffraction study of the pressure-temperature phase diagram of P$$_{2}$$O$$_{5}$$ and of the liquid P$$_{2}$$O$$_{5}$$ structure under high pressure up to 10 GPa. We found that structural transformation in the liquid P$$_{2}$$O$$_{5}$$ under pressure is unique and includes three stages: first, the disappearance of the intermediate range order of the melt together with a slow increase in the average first-coordination number $$<$$$$N$$$$_{1}$$$$>$$ (P-O and O-P neighbors) up to 4 GPa; second, the "normal" compression almost without structural modification at higher pressures up to 8-9 GPa; and, finally, the abrupt change of the short-range order structure of the liquid with the jumplike $$<$$$$N$$$$_{1}$$$$>$$ increase at 9-10 GPa.

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パーセンタイル:38.87

分野:Materials Science, Multidisciplinary

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