首页> 外文OA文献 >Single-crystal neutron diffraction study of β-Cs_3(HSO_4)_2H_(2-x)(S_xP_(1-x)O_4 (x ≃ 0.5) at 15 K
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Single-crystal neutron diffraction study of β-Cs_3(HSO_4)_2H_(2-x)(S_xP_(1-x)O_4 (x ≃ 0.5) at 15 K

机译:β-Cs_3(HSO_4)_2 H_(2-x)(S_xP_(1-x)O_4(x≃0.5)在15 K时的单晶中子衍射研究

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摘要

The structure of β-Cs_3(HSO_4)_2[H_(2-x)(S_xP_(1-x)O_4] has been examined by single-crystal neutron diffraction at 15 K. The compound crystallizes in space group C2/c and contains four formula units in the unit cell, with lattice parameters a = 19.769(9), b = 7.685(2), c = 8.858 (3) Å and β = 100.60 (4)°. Refinement of P, S and H site occupancies indicated that the value of x (in the stoichiometry) is 0.500 (6). This, together with the unit-cell volume of 1322.8(14) Å^3, implies a density of 3.463 Mg m^(-3). The structure contains zigzag rows of XO_4 anions, where X = P or S, that alternate, in a checkerboard fashion, with zigzag rows of Cs cations. Moreover, there is one proton site, H(3), with an occupancy of 0.25 and one X-atom site, X(1), that is occupied by 0.5 P and 0.5 S. These features are in general agreement with a previous X-ray structure determination carried out at 298 K. In contrast to the X-ray study, however, it was found that two different structural models adequately fit the diffraction data. In the first model, the proton vacancies and the P atoms were assumed to be randomly distributed over the H(3) and X(1) sites, respectively, and to have no impact on the local structure. In the second model, several atoms were assigned split occupancies over two neighboring sites, to reflect the presence or absence of a proton vacancy, and the presence of P or S on the X(1) site. Refinement assuming the first model, in which anisotropic displacement parameters for 12 of 14 atom sites in the asymmetric unit were employed, yielded residuals wR(F^2) = 0.084 and wR(F) = 0.038. For the second model, in which anisotropic displacement parameters were utilized for only the five atoms that were not split relative to the first model, the residuals were wR(F^2) = 0.081 and wR(F) = 0.036.
机译:β-Cs_3(HSO_4)_2 [H_(2-x)(S_xP_(1-x)O_4]的结构已通过15 K单晶中子衍射进行了研究。该化合物在C2 / c空间群中结晶并包含晶胞中的四个公式单位,晶格参数a = 19.769(9),b = 7.685(2),c = 8.858(3)Å和β= 100.60(4)°。表示x的值(按化学计量)是0.500(6)。这与1322.8(14)Å^ 3的晶胞体积一起意味着3.463 Mg m ^(-3)的密度。包含XO_4个Z型锯齿形的负离子,其中X = P或S,以棋盘格的形式交替排列,并带有Cs型锯齿形齿形;此外,还有一个质子位点H(3),占有率为0.25,一个X原子位点X(1),被0.5 P和0.5 S占据。这些特征与先前在298 K下进行的X射线结构测定总体上是一致的。但是,与X射线研究相反,发现两个不同的结构模型足够拟合衍射数据。在第一个模型中,假定质子空位和P原子分别随机分布在H(3)和X(1)位置,并且对局部结构没有影响。在第二个模型中,为几个原子分配了两个相邻位点的分裂占用率,以反映质子空位的存在与否以及X(1)位置上P或S的存在。细化假设使用第一个模型,其中使用不对称单元中14个原子位点中12个原子的各向异性位移参数,得出残差wR(F ^ 2)= 0.084和wR(F)= 0.038。对于第二个模型,其中各向异性位移参数仅用于相对于第一个模型未分裂的五个原子,残差为wR(F ^ 2)= 0.081和wR(F)= 0.036。

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    Haile S. M.; Klooster W. T.;

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