Neutrons, X-rays and Light: Scattering Methods Applied to Soft Condensed MatterP. Lindner, Th. Zemb Scattering experiments, using X-ray, light and neutron sources (in historical order) are key techniques for studying structure and dynamics in systems containing colliods, polymers, surfactants and biological macromolecules, summarized here as soft condensed matter. The education in this field in Europe is very heterogeneous and frequently inadequate, which severely limits an efficient use of these methods, especially at large-scale facilities. The series of "Bombannes" schools and the completely revised and updated second edition of the lecture notes are devoted to a practical approach to current methodology of static and dynamic techiques. Basic information on data interpretation, on the complementarity of the different types of radiation, as well as information on recent applications and developments is presented. The aim is to avoid over - as well as under-exploitation of data. |
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Results 1-3 of 81
Page 167
... phase is stable in the temperature Φς / Φο range from 25 to 32 ° C , while below 25 ° C the microemulsion phase separates with a pure oil as the second phase ( Olsson et al . , 1997 ) . The temperature dependence of the phase equilibria ...
... phase is stable in the temperature Φς / Φο range from 25 to 32 ° C , while below 25 ° C the microemulsion phase separates with a pure oil as the second phase ( Olsson et al . , 1997 ) . The temperature dependence of the phase equilibria ...
Page 377
... phase diagrams . For p2 = 0 there are only hard sphere colloids , for which a single fluid phase exists up to a colloid volume fraction = 0.49 and a solid phase above c = 0.54 with fluid - solid coexistence in between . The simulation ...
... phase diagrams . For p2 = 0 there are only hard sphere colloids , for which a single fluid phase exists up to a colloid volume fraction = 0.49 and a solid phase above c = 0.54 with fluid - solid coexistence in between . The simulation ...
Page 523
... phase , and ( b ) the product of the fraction of each phase . Since we know from WAXS that the crystallinity and the crystal structure hardly changes during the process of drawing and relaxing it can be concluded that the observed ...
... phase , and ( b ) the product of the fraction of each phase . Since we know from WAXS that the crystallinity and the crystal structure hardly changes during the process of drawing and relaxing it can be concluded that the observed ...
Contents
P N Pusey | 4 |
Shapes and Interactions | 12 |
Experimental Aspects Initial Data Reduction | 23 |
Copyright | |
18 other sections not shown
Common terms and phrases
amplitude Appl approximation average beam calculated cell Chem coefficients collimation colloidal concentration constant contrast variation correlation function corresponding Cryst crystals curvature cylinder dependence detector deuterated differential scattering cross-section dilute distance droplets dynamic light scattering effects fluctuations form factor Fourier transform Gaussian Glatter Guinier homogeneous incoherent scattering instrument interactions lamellar Lindner Macromolecules measured method micelles microemulsion microstructure molar mass molecular molecules monomers multiple scattering neutron scattering obtained optical parameter particles PDDF peak Pedersen phase photons Phys plot polydisperse polymer Porod radiation radius of gyration random walk range refractive index regime sample SAXS scattered intensity scattering angle scattering curve scattering experiments scattering function scattering length scattering length density scattering vector Schurtenberger shear shown in Fig simulations small-angle scattering solution solvent spheres spherical static light scattering structure factor surface surfactant suspension technique temperature thickness volume fraction wavelength X-ray Zemb ΦΩ