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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Page 74
... function with a periodic function system , but this is how scattering works and we do not have any other powerful physical method to study these structures . The essential effect of these differences is that in SAS we measure a ...
... function with a periodic function system , but this is how scattering works and we do not have any other powerful physical method to study these structures . The essential effect of these differences is that in SAS we measure a ...
Page 174
P. Lindner, Th. Zemb. log I ( 9 ) Scattering Function Distance Distribution Function Fourier Transform ( Rayleigh - Debye - Gans ) q min Яmax . , Inverse Scattering Problem " " Scattering Problem " ( 1 ) d Particle Autocorrelation ...
P. Lindner, Th. Zemb. log I ( 9 ) Scattering Function Distance Distribution Function Fourier Transform ( Rayleigh - Debye - Gans ) q min Яmax . , Inverse Scattering Problem " " Scattering Problem " ( 1 ) d Particle Autocorrelation ...
Page 223
... scattering , does not vanish . It is a major difference to light scattering that in general incoherent scattering ... function is related by a double Fourier transform in space and time 1 Scoh ( q , w ) = 2π farf d3r dt exp ( i ( q ...
... scattering , does not vanish . It is a major difference to light scattering that in general incoherent scattering ... function is related by a double Fourier transform in space and time 1 Scoh ( q , w ) = 2π farf d3r dt exp ( i ( q ...
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