共查询到16条相似文献,搜索用时 156 毫秒
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氟碳铈钡矿Ce2Ba3(CO3)5F2是在我国发现的新矿物,其电子衍射斑点按强度可分为两大类:较强的一类是晶体亚结构的贡献;其余衍射斑点是超结构的贡献。晶体的亚结构与黄河矿的相类似,可以划出一个六角的亚晶胞。亚晶胞参数为a0=5.06?,c0=9.63?。超结构属单斜晶系,晶胞参数为a=21.2?,b=5.06?,c=13.1?,β=95°。晶体属空间群C2/m、Cm或C2,亚结构与超结构的基矢有如下关系:该矿h00系统衍射形成的晶格象中,常夹有间距较小的条纹,或宽的黑带。本文对此进行了讨论,也讨论了该矿是否会有更大周期的超结构问题。
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本文用X射线粉末法测定了Li2K(IO3)3与Li2NH4(IO3)3的晶体结构和原子参数。发现Li3K(IO3)3,Li2NH4(IO3)3与Li2Rb(IO3)3同晶型,属单斜晶系,空间群为P21/α,每个单胞含有四个化合式量。室温的点阵常数分别为α=11.198?,b=11.046?,c=8.254?,β=111.53°,及α=11.327?,b=11.078?,c=8.341?,β=111.87°。讨论了二元化合物的形成与离子半径的关系。
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本文用差热分析、高温和室温X射线衍射分析等方法研究了Mg(IO3)2·4H2O的相变过程: Mg(IO3)2·4H2O晶体属单斜晶系,空间群为P2或Pm,每个晶胞含有两个化合式量,点阵常数为a=8.307?,b=6.627?,c=8.541?,β=1.00°45′。我们用X射线粉末法测定了α-Mg(IO3)2的晶体结构。α-Mg(IO3)2属六角晶系,其空间群是P63。在14℃的点阵参数为a=5.4777?,c=5.1282?,c/a=0.9362。每个单胞含一个化合式量,6OII占据在6(c)等效位置上,21V占据在2(b)等效位置上,Mg++无序地占据着2(a)等效位置的一半。其原子参数为xc=0.096,yc=0.344,zc=0.162,zb=0,za=0.981。从结构来看,它与α-LiIO3同晶型,所不同的是2(a)位置只有一半被Mg++离子占据着,另一半为空位。
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用低能电子衍射研究了GaAs(110)表面的弛豫。发现当理论与实验之间符合得最好时,得到的结构是,保持表面上As—Ga键长不变用一个27.32°±0.24°的旋转角(ω),使As原子向外移动0.10±0.02?,Ga原子向内移动0.55±0.02?,而从Ga到第二层时空间为d2=1.45±0.01?,从第二层Ga到第三层的空间为d3=2.01±0.01?。对此结构As的背键长lAs=2.43±0.01?(收缩0.56%),而Ga的背键长lGa=2.253±0.004?(收缩8.0%)。
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黄河矿是在我国发现的一种钡铈氟碳酸盐新矿物,其理想化学式为BaCe[Fl(CO3)2],本矿物属三方晶系,利用四圆衍射仪收集强度数据,测得α=b=5.070(±0.003)?,c=38.408(±0.005)?,空间群为R3m. z=6,本文在前人工作的基础上,对该矿物进行了较为精确的测定,最后的偏离因子R=0.041。本文还对黄河矿赝结构及超结构的关系作了探讨,与前人工作进行了对比,对类似矿物的修正方案提出看法,对个别实验数据作了讨论。
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Transmission electron microscopy (TEM) has been instrumental in advancing the field of crystalline defect analysis. Conventional TEM imaging techniques, such as bright field (BF), dark field (DF), and weak beam dark field (WBDF or g–3g) imaging, have been well-documented in the scientific literature, with simulation methods readily available for each. The present contribution highlights the use of a field-emission TEM, operated in scanning transmission electron microscopy mode, as a viable tool for defect analysis. Common techniques such as two-beam diffraction contrast and zone axis imaging are applied to defect analysis; both experimental and computational results are presented. Effects of experimental parameters such as camera length, beam divergence angle, and diffraction aperture placement are also discussed and illustrated by both experimental and computed micrographs of stacking faults. 相似文献
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Formation and microstructural investigation of Ag-Cu alloy nanoclusters embedded in SiO2 formed by sequential ion implantation 总被引:1,自引:0,他引:1
We report on the formation of alloy nanoclusters in silica by Ag/Cu ion sequential implantation. The formation of alloy nanocluster has been evidenced by optical absorption spectra, selected area electron diffraction and energy dispersive X-ray spectra. The microstructure characters of nanoclusters have been studied by high resolution transmission electron microscopy. The lattice distortion of some nanoclusters has been observed. A model has been given to explain the distortion. Some defects (partial dislocation, stacking faults) have been found in nanoclusters. 相似文献
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The role of the In/Si(111)-(4 x 1)-In surface as an atomic-scale geometrical template for the growth of Ag thin films is clarified by scanning tunneling microscopy and low energy electron diffraction. Low-temperature grown Ag films are found to have stripe structures with a transverse periodicity equal to that of indium chains of the In/Si(111)-(4 x 1)-In. The stripes exhibit a structural transformation at the thickness of 6 monolayers (ML); this relaxation allows the stripes to persist up to a thickness as large as 30 ML (approximately = 7 nm) while maintaining their mean periodicity. We attribute this stability to a coincidental matching of the periodicity and the corrugation amplitude between the Ag film and the substrate, which is realized by periodic insertion of stacking faults into a Ag fcc crystal. 相似文献