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基于61Ni同步辐射的六方结构镍基纳米颗粒的穆斯堡尔光谱

61Ni synchrotron radiation-based Mössbauer spectroscopy of nickel-based nanoparticles with hexagonal structure.

作者信息

Masuda Ryo, Kobayashi Yasuhiro, Kitao Shinji, Kurokuzu Masayuki, Saito Makina, Yoda Yoshitaka, Mitsui Takaya, Hosoi Kohei, Kobayashi Hirokazu, Kitagawa Hiroshi, Seto Makoto

机构信息

Research Reactor Institute, Kyoto University, Kumatori-cho, Sennan-gun, Osaka 590-0494, Japan.

Research and Utilization Division, Japan Synchrotron Radiation Research Institute, 1-1-1 Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5198, Japan.

出版信息

Sci Rep. 2016 Feb 17;6:20861. doi: 10.1038/srep20861.

Abstract

We measured the synchrotron-radiation (SR)-based Mössbauer spectra of Ni-based nanoparticles with a hexagonal structure that were synthesised by chemical reduction. To obtain Mössbauer spectra of the nanoparticles without (61)Ni enrichment, we developed a measurement system for (61)Ni SR-based Mössbauer absorption spectroscopy without X-ray windows between the (61)Ni84V16 standard energy alloy and detector. The counting rate of the (61)Ni nuclear resonant scattering in the system was enhanced by the detection of internal conversion electrons and the close proximity between the energy standard and the detector. The spectrum measured at 4 K revealed the internal magnetic field of the nanoparticles was 3.4 ± 0.9 T, corresponding to a Ni atomic magnetic moment of 0.3 Bohr magneton. This differs from the value of Ni3C and the theoretically predicted value of hexagonal-close-packed (hcp)-Ni and suggested the nanoparticle possessed intermediate carbon content between hcp-Ni and Ni3C of approximately 10 atomic % of Ni. The improved (61)Ni Mössbauer absorption measurement system is also applicable to various Ni materials without (61)Ni enrichment, such as Ni hydride nanoparticles.

摘要

我们测量了通过化学还原合成的具有六边形结构的镍基纳米颗粒的基于同步辐射(SR)的穆斯堡尔谱。为了获得未进行(61)Ni富集的纳米颗粒的穆斯堡尔谱,我们开发了一种用于基于(61)Ni SR的穆斯堡尔吸收光谱的测量系统,该系统在(61)Ni84V16标准能量合金和探测器之间没有X射线窗口。通过检测内转换电子以及能量标准与探测器之间的紧密接近,提高了系统中(61)Ni核共振散射的计数率。在4K下测量的光谱显示,纳米颗粒的内部磁场为3.4±0.9T,对应于0.3玻尔磁子的镍原子磁矩。这与Ni3C的值以及六方密堆积(hcp)-Ni的理论预测值不同,表明该纳米颗粒的碳含量介于hcp-Ni和Ni3C之间,约为镍原子的10%。改进后的基于(61)Ni的穆斯堡尔吸收测量系统也适用于各种未进行(61)Ni富集的镍材料,如氢化镍纳米颗粒。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7e77/4756403/7f947c42ffe7/srep20861-f1.jpg

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