Determination of triple points in the phase diagram of praseodymium.

Determination of triple points in the phase diagram of praseodymium.
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镨相图中三相点的测定。

DOI:
10.1103/physrevb.52.134
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发表时间:
1995
期刊:
Physical review. B, Condensed matter
影响因子:
--
通讯作者:
Holzapfel
Holzapfel
中科院分区:
--
文献类型:
--
作者:
Zhao;Porsch;Holzapfel

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被引文献

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采用外部加热的金刚石对顶盒装置,通过原位能量色散X射线衍射,沿着Pr(II)(fcc)、Pr(III)(扭曲的fcc)和Pr(IV)(α-铀型结构)之间的相界,研究了压力高达23 GPa、温度高达573 K的镨的相图。沿着Pr(II)(fcc)、Pr(III)(扭曲的fcc)和Pr(IV)(α-铀型结构)。这三个相的三相点位于21 GPa和537 K附近,代表在过渡到高压相Pr(IV)时Pr(II)和Pr(III)之间的明显二级相变的终点。结合Pr在室温下的压缩数据,本研究将P-T相图扩展到熔化线。
The phase diagram for praseodymium under pressures up to 23 GPa and temperatures up to 573 K is studied by in situ energy-dispersive x-ray diffraction with an externally heated diamond-anvil cell apparatus along the phase boundaries between Pr(II) (fcc), Pr(III) {distorted fcc), and Pr(IV) (a-uraniumtype structure). The triple point of these three phases is located around 21 GPa and 537 K, representing the end point of the apparently second-order phase transition between Pr{II) and Pr(III) at the transition to the high-pressure phase Pr(IV). Together with the compression data for Pr at ambient temperature, the present study extends the P-T phase diagram up to the melting lines.