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In situ X-ray diffraction measurements of the fcc-hcp phase transition boundary of an Fe-Ni alloy in an internally heated diamond anvil cell

机译:内部加热的金刚石砧室中Fe-Ni合金的fcc-hcp相变边界的原位X射线衍射测量

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The phase transition boundary between the face-centered cubic (fcc) structure and hexagonal close-packed (hcp) structure in an Fe-Ni alloy was determined at pressures from 25 to 107 GPa by using an internally resistive-heated diamond anvil cell (DAC), combined with in situ synchrotron X-ray diffraction measurements. The fcc-hcp phase transition boundary in Fe-9.7 wt% Ni is located at slightly lower temperatures than that in pure Fe, confirming the previous understanding that the addition of Ni expands the stability field of the fcc phase. The dP/dT slope of the boundary was determined to be 0.0426 GPa/K, which is slightly larger than that of pure Fe. The pressure interval of the two-phase region is about 6 GPa at a constant temperature, implying that the previous estimates by laser-heated DAC experiments of 10-20 GPa were overestimated. The two-phase region of fcc + hcp would be limited to a pressure of about 120 GPa even in Fe-15 wt%Ni, excluding the possibility of the existence of the fcc phase in the inner core if the simple linear extrapolation of the two-phase region is applied. The pressure and temperature dependences of the c/a axial ratio of the hcp phase in Fe-9.7 wt% Ni are generally consistent with those in pure Fe, suggesting that Ni has minor effects on the c/a ratio.
机译:通过使用内部电阻加热的金刚石砧盒(DAC)在25至107 GPa的压力下确定Fe-Ni合金中的面心立方(fcc)结构和六方密堆积(hcp)结构之间的相变边界),并结合原位同步加速器X射线衍射测量。 Fe-9.7 wt%Ni中的fcc-hcp相变边界位于比纯Fe中稍低的温度,这证实了先前的理解,添加Ni可以扩展fcc相的稳定性场。边界的dP / dT斜率确定为0.0426 GPa / K,比纯铁稍大。在恒定温度下,两相区域的压力间隔约为6 GPa,这意味着先前通过激光加热DAC实验得出的10-20 GPa的估计值被高估了。即使在Fe-15 wt%Ni中,fcc + hcp的两相区域也将被限制在约120 GPa的压力下,如果这两者的简单线性外推法排除在内核中存在fcc相的可能性相区域被应用。 Fe-9.7 wt%Ni中hcp相的c / a轴向比率的压力和温度依赖性通常与纯Fe中的相符,这表明Ni对c / a比率影响较小。

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