2003
DOI: 10.1051/jp4:200300016
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La diffraction des neutrons et des rayons X pour l'étude structurale des liquides et des verres

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Cited by 10 publications
(9 citation statements)
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“…[22] It is not appropriate here to go into a lengthy discussion of these corrections for either x-rays or neutrons. It will be assumed that for the various types of diffraction experiments appropriate corrections for inelasticity and other systematic effects, such as sample attenuation and multiple scattering, can be performed [23]. Even so different experimentalists often have different methods of correcting their data, so that, due to uncertainties in these corrections, independent experiments on the same material under the same conditions do not necessarily yield identical data.…”
Section: Diffraction Techniques As a Probe Of Structurementioning
confidence: 99%
“…[22] It is not appropriate here to go into a lengthy discussion of these corrections for either x-rays or neutrons. It will be assumed that for the various types of diffraction experiments appropriate corrections for inelasticity and other systematic effects, such as sample attenuation and multiple scattering, can be performed [23]. Even so different experimentalists often have different methods of correcting their data, so that, due to uncertainties in these corrections, independent experiments on the same material under the same conditions do not necessarily yield identical data.…”
Section: Diffraction Techniques As a Probe Of Structurementioning
confidence: 99%
“…Generally, this is expressed as the differential cross section, which has distinct (coherent) and self-(incoherent) scattering parts. The total interference function, F(Q), is the distinct scattering and it is convenient to use the convention of Faber-Ziman [33] to express the total interference function F(Q), in terms of a dimensionless static structure factor S(Q) [29,30]:…”
Section: Introductionmentioning
confidence: 99%
“…Short-range order is usually described by a probability function, the probability of finding an atom at a distance, r, from an atom at the origin and this is the radial distribution function q(r), often referred to as a pair distribution function. The pair distribution function is obtained by Fourier transformation of the total structure factor, S(Q), obtained from diffraction data from liquids, glasses and amorphous materials that is probed by radiation with wavelengths comparable to the inter-atomic separation [26][27][28][29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…Here Qmax and Qmin represent the upper and lower limits of the finite range in reciprocal space studied and  is the atomic number density 21 . The G(r) function emphasizes local structure.…”
Section: Methodsmentioning
confidence: 99%
“…Results are reported first as reciprocal space correlations of the total scattering (S(Q)) that represents the weighted sum of partial structure factors, expressed using the Faber-Ziman formalism 21 . The sine Fourier transform of the total, multi-component structure factor provides the total (pseudo-nuclear) pair distribution function, G(r).…”
Section: Methodsmentioning
confidence: 99%