Neutrons in Disordered Matter: Proceedings Euroconference '94 : Stockholm, Sweden, 9-13 June, 1994Monique Dahlborg, Ulf Dahlborg |
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Page 49
... scattering lengths of the com- ponents . In favourable cases the individual peaks may occur resolved in the total p ( R ) and then may be analysed , e.g. by Gauss fitting . In general a detailed investigation of the structure means the ...
... scattering lengths of the com- ponents . In favourable cases the individual peaks may occur resolved in the total p ( R ) and then may be analysed , e.g. by Gauss fitting . In general a detailed investigation of the structure means the ...
Page 61
... scattering because X - rays do not probe the light hydrogen atoms . In addition , the isotopic substitution technique by replacing hydrogen , which has a negative scattering length ( bн = -0.374 ) , by deuterium , which has a positive ...
... scattering because X - rays do not probe the light hydrogen atoms . In addition , the isotopic substitution technique by replacing hydrogen , which has a negative scattering length ( bн = -0.374 ) , by deuterium , which has a positive ...
Page 147
... scattering , via o , p . Then σ , p measures the variance of the " height " of the solid / liquid interface with ... length density profile p ( z ) . We shall primarily consider a surface layer at an interface ( z = 0 ) between a substrate ...
... scattering , via o , p . Then σ , p measures the variance of the " height " of the solid / liquid interface with ... length density profile p ( z ) . We shall primarily consider a surface layer at an interface ( z = 0 ) between a substrate ...
Common terms and phrases
Ź alloys amorphous analysis atoms behaviour binary bond angle bond length calculated carbon black chain Chem clusters configuration contribution coordination number correlation functions corresponding Cryst crystal crystalline curves determined diffraction data diffuse scattering disorder distances distribution function doped dynamics EISF elastic electronic energy EXAFS experimental data experiments fractal graphite hydration hydrogen ice Ih intensity interaction interatomic lattice layer liquid Me-O measured melt metallic glasses metalloid method molecular molecules neighbours neutron diffraction neutron scattering Ni-Nb Ni-Ni observed obtained oxygen pair correlation functions partial structure factors peak phase photons Phys Physica Scripta Physics polymer potential Q range Qmax radial distribution function Reverse Monte Carlo Rietveld refinement RMC model rotation sample scat scattering length short range order shown simulation solid structural parameters structure factor surface surfactant symmetry Table temperature tering tion titanium dioxide total structure factor X-ray