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Synchrotron X-ray Study of the Electron Density in a-Fe2O3 a-Fe2O3中电子密度的同步加速器x射线研究
Pub Date : 1994-01-01 DOI: 10.1107/s0108768194002284
E. N. Maslen, V. Streltsov, N. Streltsova, N. Ishizawa
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引用次数: 62
Tables of Coincidence Orientations for Ordered Tetragonal L lo Alloys for a Range of Axial Ratios 在一定轴向比范围内有序四边形llo合金的符合取向表
Pub Date : 1993-04-01 DOI: 10.1107/S0108768192010000
A. Singh, A. King
In this paper we develop and apply techniques for computation of CSL, DSCL and step-vector data for grain boundaries in tetragonal materials for a range of axial ratios. This has application to L10 alloys including TiA1, which is a candidate for lightweight high-temperature structural applications. Our results are compared with others and found to be more accurate and complete. We provide data for a wider range of axial ratios than those considered by previous workers. We have also derived equivalent quaternions for tetragonal crystals in tetragonalcrystal coordinates and listed conditions for selecting a unique reduced rotation in tetragonal-crystal coordinates so that a disorientation description becomes available.
在本文中,我们开发和应用的技术计算CSL, DSCL和步进矢量数据的晶界四边形材料在一定范围的轴向比。这适用于L10合金,包括TiA1,它是轻质高温结构应用的候选材料。将我们的结果与他人的结果进行比较,发现我们的结果更加准确和完整。我们提供的数据更广泛的轴向比比那些考虑到以前的工人。我们还推导了四边形晶体在四边形晶体坐标中的等效四元数,并列出了在四边形晶体坐标中选择唯一的减少旋转的条件,以便可以进行定向失位描述。
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引用次数: 8
Arithmetic equivalence of point groups for quasiperdiodic structures 准周期结构点群的算术等价
Pub Date : 1993-03-01 DOI: 10.1107/S0108767392008845
F. Wijnands, T. Janssen
Necessary and sufficient conditions are formulated for an n-dimensional arithmetic point group such that it may be the symmetry group of a d-dimensional quasiperiodic but not periodic, i.e. incommensurate, structure with Fourier modulus of rank n. Only point groups leaving invariant a d-dimensional subspace (the physical space) are considered. For an arithmetic point group describing an incommensurate structure, all equivalent choices for the internal space are related by the normalizer in Gl (n, bb Z) of the point group. Also, the conditions on arithmetic equivalence of two point groups allowing an incommensurate structure are discussed. These conditions yield a further partition of the arithmetic crystal classes.
给出了一个n维算术点群的充分必要条件,使得它可以是d维拟周期而非周期的对称群,即n阶傅里叶模的不相称结构。只考虑点群在d维子空间(物理空间)中保持不变。对于描述不相称结构的算术点群,内部空间的所有等价选择都由点群的Gl (n, bb Z)中的归一化器联系起来。并讨论了允许不相称结构的两个点群的算术等价条件。这些条件产生算术晶体类的进一步划分。
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引用次数: 3
Structure of Bis(n-butylammonium) Tetrachlorocadmate(II) 四氯酸双(正丁铵)的结构
Pub Date : 1992-07-15 DOI: 10.1107/S010827019101452X
B. Doudin, G. Chapuis
Cristallisation dans Abma avec a = 7,538, b = 7,416 et c = 30,803 A, Z = 4; affinement jusqu'a R = 0,045. Cette phase lamellaire est semblable a la phase δ observee dans les composes parents, avec une inclinaison des octaedres CdCl 6 favorisant une liaison hydrogene specifique avec la fin ammonium des chaines aliphatiques. Aucun modele simple ne peut expliquer de facon convaincante le desordre des chaines, contrairement a ce qui avait ete le cas pour l'equivalent Mn. Observations de transitions de phase autour de 200 K.
在Abma中结晶,a = 7,538, b = 7,416, c = 30,803 a, Z = 4;细化至R = 0.045。这种层状相类似于在母体化合物中观察到的δ相,cdcl6八面体的倾斜度有利于与脂肪链的铵端形成特定的氢键。没有一个简单的模型可以令人信服地解释链的无序,不像等效Mn的情况。观测到200 K左右的相变。
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引用次数: 6
A position-space model for superconductivity in Y Ba2 Cu3O7-x yba2cu3o7 -x超导的位置-空间模型
Pub Date : 1992-02-01 DOI: 10.1107/S0108768191010509
E. N. Maslen, N. Spadaccini
Cristallisation dans Pmmm avec a = 3,847, b = 3,875 et c = 11,70 A (ensemble de donnees 1), a = 3,842, b = 3,886 et c = 11,690 A (ensemble de donnees 2), Z = 1; affinement jusqu'a R = 0,041 (O5 exclu) et R = 0,040 (O5 inclus). Discussion detaillee des cartes de distribution de la charge electronique et etablissement d'un modele de la supraconductivite.
在Pmmm中结晶,a = 3.847, b = 3.875和c = 11.70 a(数据集1),a = 3.842, b = 3.886和c = 11.690 a(数据集2),Z = 1;精炼至R = 0.041(不包括O5)和R = 0.040(包括O5)。详细讨论了电子电荷分布图和超导性模型的建立。
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引用次数: 5
On the Refinement on Profile, Background and Net Intensities 关于轮廓、背景和净强度的细化
Pub Date : 1991-03-01 DOI: 10.1107/S0108767390011308
D. Schwarzenbach, H. Flack
The raw data obtained with a single-crystal diffractometer are typically integrated profile and background intensities. All linear combinations of these data items, and in particular net intensities and total backgrounds, are equivalent observations. However, net intensities may be negative, in apparent contradiction with basic physics. Backgrounds are generally discarded from the list of observations once they have been subtracted from the profile intensities. In a crystal structure refinement on all observations, structural parameters including scale, extinction and possibly others, as well as individual background intensities, are refined on the observed profile intensities and on the observed background intensities. It is shown that, in such a refinement, the structural parameters are determined exclusively by the net intensities as in traditional least squares, whereas calculated backgrounds depend on the difference between observed and calculated net intensities. Negative net intensities are therefore not in contradiction with physics or with the structural model, and should be retained unaltered in the data set.
单晶衍射仪获得的原始数据通常是轮廓和背景强度的综合数据。这些数据项的所有线性组合,特别是净强度和总背景,都是等效的观测值。然而,净强度可能是负的,这显然与基础物理学相矛盾。背景一旦从剖面强度中减去后,通常从观测列表中丢弃。在所有观测的晶体结构精化中,结构参数包括尺度、消光和可能的其他参数,以及单个背景强度,都是根据观测到的剖面强度和观测到的背景强度进行精化的。结果表明,在这种细化中,结构参数完全由传统最小二乘法中的净强度决定,而计算背景取决于观测和计算净强度之间的差异。因此,负净强度与物理或结构模型并不矛盾,应在数据集中保持不变。
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引用次数: 7
Limits of the Patterson Method for the Determination of one-dimensionally Modulated Structures 帕特森法测定一维调制结构的局限性
Pub Date : 1989-01-01 DOI: 10.1107/S0108767388013844
B. Doudin, G. Chapuis
The Patterson function can reveal the modulation of a basic structure if its summation terms include only satellite reflections. Examples of Patterson summations for various types of modulated structures illustrate the difficulties of interpretation and the bias occurring in the determination of the amplitudes and phases of the modulation. The opportunity to use the Patterson function to determine modulated structure is discussed.
如果帕特森函数的和项仅包含卫星反射,则可以揭示基本结构的调制。各种类型调制结构的帕特森求和的例子说明了解释的困难和在确定调制的幅度和相位时发生的偏差。讨论了利用帕特森函数确定调制结构的可能性。
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引用次数: 3
Structure of the 4:3 Complex Between Gadolinium Nitrate and 18-Crown-6 Ether: [Gd(NO3)2(C12H24O6)]3[Gd(NO3)6] 硝酸钆与18-冠-6醚4:3配合物的结构:[Gd(NO3)2(C12H24O6)]3[Gd(NO3)6]
Pub Date : 1988-10-15 DOI: 10.1107/S0108270188006651
F. Nicolò, J. Bünzli, G. Chapuis
Le compose du titre cristallise dans C2 avec affinement jusqu'a 0,049. Le complexe est constitue d'anion [Gd(NO 3 ) 6 ] 3− de symetrie 2 et de deux types de cations [Gd(NO 3 ) 2 (18-crown-6)] + , l'un en position speciale de symetrie 2, l'autre en position generale. Ces trois ions etant dans le rapport 1:1:2
滴定物在C2处结晶,精细度可达0.049。该配合物由对称2的阴离子[Gd(no3) 6] 3−和两种阳离子[Gd(no3) 2(18-皇冠-6)]+组成,一种位于特殊对称2位置,另一种位于一般位置。这三个离子的比例是1:1:2
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引用次数: 9
On the Use of Least-Squares Restraints for Origin Fixing in Polar Space Groups 极坐标空间群原点固定的最小二乘约束
Pub Date : 1988-07-01 DOI: 10.1107/S0108767388002697
H. Flack, D. Schwarzenbach
The theory of fixing the origin of the coordinate system in a polar space group by use of restraints (soft constraints or pseudo-observations) is developed for any space group in any setting. The coefficients of the optimal restraint equation are on the average proportional to the square of the atomic numbers. They are determined directly from the unrestrained singular normal-equations matrix. Application of the restraint results in a positive-definite matrix which is as nearly diagonal as possible for the atomic positional coordinates along the origin-free axes. Correlations between these coordinates are therefore minimized. A very compact completely general and easily implemented algorithm results which functions without user intervention.
提出了利用约束(软约束或伪观测)在极空间群中固定坐标系原点的理论,适用于任何环境下的任何空间群。最优约束方程的系数平均与原子序数的平方成正比。它们是直接由无约束奇异正态方程矩阵确定的。约束的应用使原子位置坐标沿无原点轴的正定矩阵尽可能接近对角。因此,这些坐标之间的相关性被最小化。一个非常紧凑、完全通用且易于实现的算法,其功能无需用户干预。
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引用次数: 117
Structure of Dibromo(thiosemicarbazide)cadmium(II) Monohydrate 二溴(硫代氨基脲)镉(II)一水化合物的结构
Pub Date : 1988-06-15 DOI: 10.1107/S0108270188000885
F. Nicolò, H. E. Ghaziri, G. Chapuis
[CdBr 2 (SCN 3 H 5 )]•H 2 O cristallise dans le systeme monoclinique avec le groupe d'espace Ia. Affinement de la structure jusqu'a 0,031. La geometrie de coordination autour de Cd est un octaedre forme par 2 atomes Br, 3 atomes S et 1 atome N
[cdbr2 (SCN 3h5)]•h2 O在空间群Ia的单斜系统中结晶。结构细化至0.031。Cd周围的配位几何是由2个Br原子、3个S原子和1个N原子组成的八面体
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引用次数: 3
期刊
Acta Crystallographica
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