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arXiv 1409.4902cond-mat.mtrl-sci
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化学计量比Ni2MnGa铁磁记忆合金的无公度调制

Incommensurate modulations in stoichiometric Ni2MnGa ferromagnetic shape memory alloy: An overview

Sanjay Singh, S. R. Barman, D. Pandey

摘要:

本文简要介绍了我们最近利用高分辨同步辐射X射线粉末衍射谱对Ni 2 MnGa铁磁记忆合金的预马氏体和马氏体相的长周期调制性质的研究工作。使用Pnnm空间群的相称结构模型无法正确解释由于调制而出现的卫星反射的峰值位置。LeBail和Rietveld使用(3+1)-D超空间群$Immm(00γ)s00$的改进表明,所有反射的峰位置,包括卫星,可以令人满意地解释为预马氏体和马氏体相的无公度调制。无公度调制矢量为q= 0.33761(5)c* =(1/3+ $δ$ 1)c* 和0.43160(3)c*=(3/7+ $δ$ 2)c*,其中$δ$ 1和$δ$ 2分别为预马氏体和马氏体相的膨胀度。预马氏体和马氏体相的最近有理近似的周期分别被确认为3 M和7 M,与单晶衍射结果一致。

英文摘要:

This article presents a brief overview of our recent work on the nature of long period modulation in the premartensite and martensite phases of Ni2MnGa ferromagnetic shape memory alloy using high resolution synchrotron x-ray powder diffraction patterns. The commensurate structure model using the Pnnm space group is unable to account for the peak positions of the satellite reflections that appear due to modulations correctly. LeBail and Rietveld refinements using the (3+1)-D super space group $Immm(00γ)s00$ show that the peak positions of all the reflections, including the satellites, can be explained satisfactorily using incommensurate modulations for both the premartensite and martensite phases. The incommensurate modulation vectors are found to be q= 0.33761(5)c* = (1/3+$δ$1)c* and 0.43160(3)c*= (3/7+$δ$2)c*, where $δ$1 and $δ$2 are the degrees of incommensuration for the premartensite and martensite phases, respectively. The periodicity of the closest rational approximant of the premartensite and martensite phases are confirmed to be 3M and 7M, respectively, in agreement with single crystal diffraction results.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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