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A high resolution synchrotron x-ray powder diffraction study of the incommensurate modulation in the martensite phase of Ni2MnGa: Evidence for nearly 7M modulation and phason broadening

机译:高分辨率同步辐射X射线粉末衍射研究   Ni2mnGa马氏体相中的不相称调制:证据   近7m调制和phason展宽

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摘要

The modulated structure of the martensite phase of Ni2MnGa is revisited usinghigh resolution synchrotron x-ray powder diffraction (SXRPD) measurements,which reveals higher order satellite reflections up to the 3rd order and phasonbroadening of the satellite peaks. The structure refinement, using the (3+1)dimensional superspace group approach, shows that the modulated structure ofNi2MnGa can be described by orthorhombic superspace group Immm(00$\gamma$)s00with lattice parameters a= 4.21861(2) {\AA}, b= 5.54696(3) {\AA}, and c=4.18763(2) {\AA} and an incommensurate modulation wave vector q= 0.43160(3)c*=(3/7+$\delta$)c*, where $\delta$=0.00303(3) is the degree of incommensurationof the modulated structure. Additional satellite peak broadening, which couldnot be accounted for in terms of the anisotropic strain broadening based on alattice parameter distribution , has been modeled in terms of phasons usingfourth rank covariant strain tensor representation for incommensuratestructures. The simulation of single crystal diffraction patterns from therefined structural parameters unambiguously reveals a rational approximantstructure with 7M modulation. The inhomogeneous displacement of differentatomic sites on account of incommensurate modulation and the presence of phasonbroadening clearly rule out the adaptive phase model proposed recently byKaufmann et al.[1] and suggests that the modulation in Ni2MnGa originates fromsoft-mode phonons.
机译:通过高分辨率同步加速器X射线粉末衍射(SXRPD)测量,重新研究了Ni2MnGa的马氏体相的调制结构,该结构揭示了直至三阶的高阶卫星反射和卫星峰的声波展宽。使用(3 + 1)维超空间群方法对结构进行细化,表明Ni2MnGa的调制结构可以用正交晶格超空间群Immm(00 $ \γ$)s00来描述,其晶格参数为a = 4.21861(2){\ AA} ,b = 5.54696(3){\ AA},而c = 4.18763(2){\ AA},调制波向量q = 0.43160(3)c * =(3/7 + $ \ delta $)c * ,其中$ \ delta $ = 0.00303(3)是调制结构的不相称程度。已使用四阶协变应变张量表示法针对不相称的结构对相位进行了建模,从而无法通过基于晶格参数分布的各向异性应变扩展来解释其他卫星峰值扩展。从确定的结构参数对单晶衍射图进行的模拟清楚地揭示了具有7M调制的合理近似结构。由于不适当的调制,不同原子位点的不均匀位移以及声相展宽的存在清楚地排除了Kaufmann等人[1]最近提出的自适应相位模型。并暗示Ni2MnGa中的调制源于软模声子。

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