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  • 1
    Online Resource
    Online Resource
    Oxford :Oxford University Press, Incorporated,
    Keywords: X-ray crystallography. ; Crystals -- Structure. ; Powders -- Optical properties -- Measurement. ; Electronic books.
    Description / Table of Contents: Our understanding of the properties of materials, from drugs and proteins to catalysts and ceramics, is almost always based on structural information. This book describes the new developments in powder diffraction which make it possible for scientists to obtain such information. This book guides both novices and experienced practitioners through the maze of possibilities.
    Type of Medium: Online Resource
    Pages: 1 online resource (358 pages)
    Edition: 1st ed.
    ISBN: 9780191525568
    Series Statement: International Union of Crystallography Monographs on Crystallography Series ; v.13
    DDC: 548.9
    Language: English
    Note: Intro -- Contents -- List of contributors -- 1 Introduction -- 1.1 Crystal structures from powder diffraction data -- 1.2 The structure determination process -- 1.3 Adapting single-crystal structure solution methods to powder diffraction data -- 1.4 Direct-space methods that exploit chemical knowledge -- 1.5 Hybrid approaches -- 1.6 Outlook -- Acknowledgements -- References -- 2 Structure determination from powder diffraction data: an overview -- 2.1 Introduction -- 2.2 Early history of powder diffraction -- 2.3 Early ab initio approaches -- 2.4 Pre-Rietveld refinement methods -- 2.5 Rietveld refinement -- 2.6 Solving unknown structures from powder data -- 2.7 Trial-and-error and simulation methods -- 2.8 Some examples of structure determination from powder data -- 2.9 Conclusions -- References -- 3 Laboratory X-ray powder diffraction -- 3.1 Introduction -- 3.2 The reflection overlap problem -- 3.2.1 Instrumental broadening-g(2& -- #952 -- ) -- 3.2.2 Sample broadening-f[sub(hkl)](2& -- #952 -- ) -- 3.2.3 H(x) profiles -- 3.3 Instrumentation and experimental considerations -- 3.3.1 Diffractometer geometries -- 3.3.2 Monochromatic radiation -- 3.3.3 Data quality -- 3.4 Examples of crystal structure solution -- 3.4.1 Bragg-Brentano powder diffraction data -- 3.4.2 Debye-Scherrer powder diffraction data -- 3.5 Conclusions -- Acknowledgements -- References -- 4 Synchrotron radiation powder diffraction -- 4.1 Introduction -- 4.2 Synchrotron powder diffraction instruments in use for ab initio structure determination -- 4.3 Angular resolution, lineshape and choice of wavelength -- 4.4 Data preparation and indexing -- 4.5 Pattern decomposition and intensity extraction -- 4.6 Systematic errors -- 4.6.1 Particle statistics -- 4.6.2 Preferred orientation -- 4.6.3 Absorption -- 4.6.4 Extinction -- 4.7 Examples of structure solution. , 4.7.1 Pioneering studies -- 4.7.2 Organic compounds -- 4.7.3 Microporous materials -- 4.7.4 Organometallics -- 4.7.5 More difficult problems -- 4.8 Conclusions -- Acknowledgements -- References -- 5 Neutron powder diffraction -- 5.1 Introduction -- 5.2 Instrumentation -- 5.3 Autoindexing and space group assignment -- 5.4 Patterson methods -- 5.5 Direct methods -- 5.6 X-n structure solution -- 5.7 Future possibilities -- References -- 6 Sample preparation, instrument selection and data collection -- 6.1 Introduction -- 6.2 Issues and early decisions-experimental design -- 6.3 Multiple datasets -- 6.4 The sample -- 6.4.1 Sources of sample-related errors -- 6.4.2 Number of crystallites contributing to the diffraction process -- 6.4.3 Increasing the number of crystallites examined -- 6.4.4 Generating random orientation -- 6.4.5 Removing extinction -- 6.5 The instrument -- 6.5.1 What radiation to use-X-rays or neutrons? -- 6.5.2 What wavelength to use? -- 6.5.3 Number of 'independent' observations (integrated intensities) -- 6.5.4 What geometry to use? -- 6.5.5 Sources of instrument-related error -- 6.6 Data collection -- 6.6.1 Step time and width recommendations -- 6.6.2 Variable counting time data collection -- 6.7 Conclusions -- References -- 7 Autoindexing -- 7.1 Introduction -- 7.2 Basic relations -- 7.3 The indexing problem -- 7.4 The dominant zone problem -- 7.5 Geometrical ambiguities-derivative lattices -- 7.6 Errors in measurements -- 7.7 Indexing programs -- 7.7.1 ITO -- 7.7.2 DICVOL91 -- 7.7.3 TREOR90 -- 7.7.4 Why more than one indexing program? -- 7.8 Computing times -- 7.9 The PDF 2 database -- 7.10 Comments -- Appendix: (Most likely) unit-cell dimensions for selected PDF-2 powder patterns -- References -- 8 Extracting integrated intensities from powder diffraction patterns -- 8.1 Introduction -- 8.2 The Le Bail method. , 8.2.1 The origins of the Le Bail method -- 8.2.2 The iterative Le Bail algorithm -- 8.3 The Pawley method -- 8.3.1 Introduction -- 8.3.2 Mathematical background -- 8.4 Space group determination -- 8.5 Overcoming Bragg peak overlap -- 8.6 Incorporating crystallographic information -- 8.7 Conclusions -- Acknowledgements -- References -- 9 Experimental methods for estimating the relative intensities of overlapping reflections -- 9.1 Introduction -- 9.2 Anisotropic thermal expansion -- 9.2.1 A simple two-peak analysis -- 9.2.2 Mathematical aspects of the analysis of integrated intensities collected at more than one temperature -- 9.2.3 An example of differential thermal expansion-chlorothiazide -- 9.3 Texture -- 9.3.1 Concept -- 9.3.2 Sample preparation -- 9.3.3 Texture description -- 9.3.4 Instrumentation -- 9.3.5 Data collection -- 9.3.6 Data analysis -- 9.3.7 Example -- 9.4 Conclusions -- References -- 10 Direct methods in powder diffraction-basic concepts -- 10.1 Introduction -- 10.2 Basics of Direct methods -- 10.3 Direct methods in practice -- 10.3.1 Normalization and setting up phase relations -- 10.3.2 Selection of starting-set phases -- 10.3.3 Active phase extension -- 10.3.4 Selection of most likely numerical starting set (criteria) -- 10.4 Whole-pattern fitting -- 10.4.1 The Pawley whole-pattern refinement -- 10.4.2 The two-step LSQPROF whole-pattern fitting procedure -- 10.5 Estimation of the intensity of completely overlapping reflections: the DOREES program -- 10.6 Direct methods for powder data in practice: the POWSIM package -- References -- 11 Direct methods in powder diffraction-applications -- 11.1 Introduction -- 11.2 A set of test structures -- 11.3 Performance of extraction algorithms -- 11.4 Some warnings about the use of powder data -- 11.5 Powder pattern decomposition using supplementary prior information. , 11.5.1 Pseudo-translational symmetry -- 11.5.2 Expected positivity of the Patterson function in reciprocal space -- 11.5.3 The expected positivity of the Patterson function in direct space -- 11.5.4 A located molecular fragment -- 11.6 Applications -- References -- 12 Patterson methods in powder diffraction: maximum entropy and symmetry minimum function techniques -- 12.1 Introduction -- 12.2 The crystal structure and its Patterson function -- 12.2.1 Patterson maps calculated from X-ray powder diffraction data -- 12.2.2 Patterson maps calculated from neutron powder diffraction data -- 12.3 Conventional methods for improving the interpretability of the Patterson map -- 12.4 Maximum entropy Patterson maps -- 12.5 Decomposition of overlapping Bragg peaks using the Patterson function -- 12.6 Solving a crystal structure directly from a powder Patterson map -- 12.7 Automatic location of atomic positions with the symmetry minimum function -- 12.8 Examples of structure solution using automated Patterson superposition techniques -- 12.8.1 Bismuth nitride fluoride Bi[sub(3)]NF[(sub(6)] -- 12.8.2 Synthetic CaTiSiO[(sub(5)] -- Acknowledgements -- References -- 13 Solution of Patterson-type syntheses with the Direct methods sum function -- 13.1 Introduction -- 13.2 Definition of the modulus sum function -- 13.3 The modulus sum function in reciprocal space -- 13.4 The sum function tangent formula, S' - TF -- 13.5 Application of the sum function tangent formula to powder diffraction data -- Acknowledgements -- References -- 14 A maximum entropy approach to structure solution -- 14.1 Introduction -- 14.2 Data collection, range and overlap -- 14.3 Starting set choices: defining the origin and enantiomorph -- 14.4 Basis set expansion and the phasing tree -- 14.5 Log-likelihood gain -- 14.6 Centroid maps -- 14.7 Fragments and partial structures. , 14.8 Using likelihood to partition overlapped reflections -- 14.8.1 The overlap problem defined in terms of hyperphases and pseudophases -- 14.8.2 Duncan's procedure for multiple significance tests -- 14.8.3 The determination of pseudophases using the maximum entropy-likelihood method and Duncan's procedure -- 14.9 The maximum entropy method and the need for experimental designs -- 14.9.1 Error correcting codes and their use in MICE -- 14.10 Conclusions and other possibilities -- Acknowledgements -- References -- 15 Global optimization strategies -- 15.1 Introduction -- 15.2 Background -- 15.3 Describing a crystal structure -- 15.4 Calculating the odds -- 15.5 Beating the odds-global optimization algorithms -- 15.5.1 A search method with a physical basis-simulated annealing -- 15.5.2 A search method with a biological basis-genetic algorithms -- 15.5.3 Search methods with a social basis-the swarm -- 15.5.4 The downhill simplex algorithm-a 'semi-global' optimizer -- 15.5.5 Other approaches -- 15.5.6 Which algorithm is best? -- 15.5.7 Use of molecular envelope information -- 15.5.8 Hybrid DM-global optimization approaches -- 15.6 Structure evaluation-the cost function -- 15.6.1 Efficiency of function evaluations -- 15.6.2 Multi-objective optimization -- 15.6.3 Maximum likelihood -- 15.7 Examples -- 15.8 Influence of crystallographic factors -- 15.9 Caveats and pitfalls -- 15.10 Conclusions -- Acknowledgements -- References -- 16 Solution of flexible molecular structures by simulated annealing -- 16.1 Introduction -- 16.2 Simulated annealing -- 16.3 Constraints and restraints -- 16.3.1 Non-structural constraints -- 16.3.2 Structural restraints -- 16.3.3 Molecular crystals -- 16.4 Examples -- 16.4.1 (PEO)[sub(3)]:LiN(SO[sub(2)]CF[sub(3)])[sub(2)] -- 16.4.2 PEO:NaCF[sub(3)]SO[sub(3)] -- 16.4.3 PEO[sub(6)]:LiAsF[sub(6)] -- 16.5 Discussion. , Acknowledgements.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 2473-2480 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The rotational potential of methyl groups in p-xylene is calculated from transferable pair interaction potentials on the basis of the low temperature crystal structure. Various parametrizations of pair potentials are used. Rotational states in these potentials are calculated and compared to tunneling and librational transitions observed by inelastic neutron scattering. None of the pair interaction potentials can describe the rotational modes correctly. The best results are obtained with Williams IVb parameters. Improvement could be achieved by diminishing the hydrogen–hydrogen interaction strength at short distances.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 5653-5661 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The crystal structure of α-phase toluene at 5 K has been refined from high resolution neutron powder diffraction data and the charge distribution in the molecule calculated ab initio. From these data, methyl rotational potentials of the two inequivalent methyl groups have been calculated for various parametrizations of transferable pair potentials and compared with potentials derived from tunneling and librational transitions. The results demonstrate that the inclusion of Coulomb interactions is necessary to reproduce the equilibrium orientations of the methyl groups. However, none of the model pair potentials yield the very strong sixfold contribution of the rotational potential of methyl group 1. The best approximation to the experimentally determined values is obtained with the pair potential parameters of Kitaigorodskii [Acta Crystallogr. 18, 585 (1965)]. However, by the inclusion of existing results on p-xylene, the average agreement obtained with the parametrization of Claverie [Acta Crystallogr. Part A 31, 448 (1975)] is equally good. Overall, it was found that general improvements can be made if the repulsive parts of the model pair potentials are softened. The presence of two inequivalent methyl groups in toluene which are influenced in different ways by the various contributions to the interaction provides a rigorous test of the modeling techniques.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 5084-5087 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Intermetallic compounds of the type RE(TM1−xMx)12 with RE=Y, Er; TM=Fe, Co; M=Si, Ti, V of the ThMn12 tetragonal crystal structure have been studied by the singular point detection technique and high-resolution neutron powder diffraction in order to (a) evaluate both the rare-earth and transition-metal sublattice contributions to the magnetocrystalline anisotropy, (b) compare the Fe and Co anisotropies in the ThMn12 structure, and (c) to verify the existence of any preferential entrance in the transition metal sublattice for various stabilizing ions. The transition metal anisotropy is of the same type (Fe axial, Co planar) and magnitude as in RE2Fe14B compounds. However, there is no anomalous temperature behavior of the anisotropy field Ha. With decreasing temperature, the value of Ha increases from 21 kOe at 293 K to 37 kOe at 78 K in YFe11Ti. Similar values are obtained for other Fe-based compounds. The contribution of Er to the anisotropy is found to be surprisingly low. The anisotropy field of ErFe11Ti varies from 24 kOe at 293 K to 63 kOe at 100 K. The observed low values of the Curie temperatures in these compounds appears once again to limit their use in possible applications. Neutron powder diffraction shows that the 8j and 8f sites of the ThMn12 structure are virtually fully occupied by Fe, while the 8i site is partially occupied by Fe and V in YFe10V2.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Chemistry of materials 1 (1989), S. 237-240 
    ISSN: 1520-5002
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 14167-14173 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 1520-5002
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 34 (2001), S. 691-698 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A modified least-squares analysis is presented that allows reliable structural parameters to be extracted from a powder diffraction pattern even in the presence of a substantial unmodelled impurity contribution. The algorithm is developed within the context of Bayesian probability theory. Experimental points that fall above those calculated, and are thus more probably from impurity peaks, are systematically down-weighted. This approach is illustrated with a two-phase example.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 18 (1985), S. 461-466 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The Voigt function has been incorporated as a peak-shape description into a program for the refinement of constant-wavelength X-ray and neutron diffraction patterns. The results obtained for neutron diffraction are encouraging and indicate that the Voigt function describes the symmetrical component of the profile peak shape to high accuracy even in the presence of substantial line broadening from particle-size effects. In contrast with approximations to the Voigt function, such as the pseudo-Voigt and Pearson VII functions, the present treatment allows the angular dependences of line-broadening effects resulting from particle-size and instrumental contributions to be coded independently from each other in the Rietveld technique. The present treatment, which details improvements to the symmetrical component of the peak shape, does not offer a fully rigorous description of the peak shape as asymmetry corrections such as those given by Howard [J. Appl. Cryst. (1982), 15, 615–620] are not included.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 19 (1986), S. 63-64 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The Voigt function is now recognized to be one of the best mathematical descriptions of the symmetrical component of the peak shape in constant-wavelength X-ray and neutron powder diffraction. The simpler pseudo-Voigt function has been used previously to provide an empirical fit to observed peak shapes. In this paper, a parameterization of this function is obtained to make it, to a very good approximation, equivalent to a Voigt function, and, additionally, it is described by the half-width parameters of the Gaussian and Lorentzian components of that Voigt function. This new construction allows for greater flexibility in peak-shape description and, in particular, allows for a more straightforward convolution of additional functional contributions into the `Voigt' component of a peak shape description.
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