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在高达332吉帕斯卡压力下,冲击镍中面心立方相的稳定性。

Stability of the fcc phase in shocked nickel up to 332 GPa.

作者信息

Pereira Kimberly A, Clarke Samantha M, Singh Saransh, Briggs Richard, McGuire Christopher P, Lee Hae Ja, Khaghani Dimitri, Nagler Bob, Galtier Eric, Cunningham Eric, McGonegle David, Tracy Sally J, Vennari Cara, Gorman Martin G, Coleman Amy L, Davis Carol, Hutchinson Trevor, Eggert Jon H, Smith Raymond F, Walsh James P S

机构信息

Department of Chemistry, University of Massachusetts Amherst, Amherst, MA, USA.

Lawrence Livermore National Laboratory, Livermore, CA, USA.

出版信息

Nat Commun. 2025 May 12;16(1):4385. doi: 10.1038/s41467-025-59385-y.

DOI:10.1038/s41467-025-59385-y
PMID:40355474
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12069704/
Abstract

Despite making up 5-20 wt.% of Earth's predominantly iron core, the melting properties of elemental nickel at core conditions remain poorly understood, due largely to a dearth of experimental data. We present here an in situ X-ray diffraction study performed on laser shock-compressed samples of bulk nickel, reaching pressures up to  ~ 500 GPa. Hugoniot states of nickel were targeted using a flat-top laser drive, with in situ X-ray diffraction data collected using the Linac Coherent Light Source. Rietveld methods were used to determine the densities of the shocked states from the measured diffraction data, while peak pressures were determined using a combination of measured particle velocities, shock transit times, hydrodynamic simulations, and laser intensity calibrations. We observed solid compressed face-centered cubic (fcc) Ni up to at least 332 ± 30 GPa along the Hugoniot-significantly higher than expected from the majority of melt lines that have been proposed for nickel. We also bracket the partial melting onset to between 377 ± 38 GPa and 486 ± 35 GPa.

摘要

尽管镍元素在地球主要由铁构成的地核中占5%-20%(重量),但在核条件下元素镍的熔化特性仍知之甚少,这主要是由于缺乏实验数据。我们在此展示了一项对块状镍的激光冲击压缩样品进行的原位X射线衍射研究,压力高达约500吉帕。使用平顶激光驱动来确定镍的雨贡纽状态,并利用直线加速器相干光源收集原位X射线衍射数据。利用Rietveld方法从测量的衍射数据中确定冲击状态的密度,而峰值压力则通过测量粒子速度、冲击渡越时间、流体动力学模拟和激光强度校准相结合的方式来确定。我们观察到沿着雨贡纽曲线,固态压缩的面心立方(fcc)镍至少在332±30吉帕时仍保持固态——这比大多数已提出的镍的熔化线所预期的要高得多。我们还确定了部分熔化开始的压力范围在377±38吉帕至486±35吉帕之间。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/6e80d56e1909/41467_2025_59385_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/daaaf259b83b/41467_2025_59385_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/792d456debe2/41467_2025_59385_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/620fdd0a2987/41467_2025_59385_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/28f2fce49187/41467_2025_59385_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/6e80d56e1909/41467_2025_59385_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/daaaf259b83b/41467_2025_59385_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/792d456debe2/41467_2025_59385_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/620fdd0a2987/41467_2025_59385_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/28f2fce49187/41467_2025_59385_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/67f8/12069704/6e80d56e1909/41467_2025_59385_Fig5_HTML.jpg

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本文引用的文献

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Unveiling the effect of Ni on the formation and structure of Earth's inner core.揭示镍对地球内核形成和结构的影响。
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Melting of Tantalum at Multimegabar Pressures on the Nanosecond Timescale.纳秒时间尺度下多兆巴压力下钽的熔化
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Crystal Structure and Melting of Fe Shock Compressed to 273 GPa: In Situ X-Ray Diffraction.铁冲击压缩至273吉帕斯卡时的晶体结构与熔化:原位X射线衍射
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