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Neutron reflection amplitude

Figs. 7 and 8 respectively show the ripples obtained by SIMS and neutron reflection during welding of HDH/DHD interfaces. Its interesting to note that all dynamics models predict ripples since in general, the chain ends move faster than the chain centers. However, their shape, amplitude and time dependence provide a... [Pg.364]

A neutron reflectometer utilizes the optical phenomenon that neutrons incident on the material surface undergo refraction and reflection if the refractive indices on each side of the surface interface are different. A neutron interferometer using a perfect silicon crystal is analogous to the Mach-Zender interferometer of classical optics. The neutron wave amplitude coherently split by the Bragg reflection is superposed again at the second beam splitter and... [Pg.32]

The second series of results that we present have been obtained by small-angle neutron scattering (SANS). Contrary to the EWIF method and to the neutron-reflectivity technique, SANS does not deal with a single, flat, well oriented, small surface but need a large amount of interface coated by polymer. The polymer substrate is therefore a porous medium or a colloidal suspension. For such samples, the scattered intensity i(q) per unit volume (in cm" ) is the sum of three terms resulting from the interferences between the amplitudes scattered by the solid and by the polymer. [Pg.72]

The structure factor S(q as defined in Eq. (54) in terms of the Ising pseudospins Si, in the framework of the first Bom approximation describes elastic scattering of X-rays, neutrons, or electrons, from the adsorbed layer. SCq) is particularly interesting, since in the thermodynamic limit it allows to estimate both the order parameter amplitude tj/, the order parameter susceptibility X4, and correlati length since for q near the superstructure Bragg reflection q we have (k = q— q%)... [Pg.130]

The advantage of using polarized neutrons to determine weak magnetic reflections is clearly apparent. For example, if T =0.01 then the magnetic contribution to the intensity in an unpolarized beam experiment is 0.01 percent, but R Ri 1.04, i.e., there is a 4 percent effect on changing the incident neutron polarization. It is necessary to know the nuclear scattering amplitude accurately if an accurate magnetic amplitude is to be obtained and extinction corrections in particular must be accurately performed. [Pg.32]

The procedure can be expanded in a piecewise fashion [17,18] to obtain the reflection and transmission amplitudes arising from the reflection of neutrons from an arbitrary potential or SLD profile if the potential is divided into a discrete number (j) of rectangular lamellae. The reflection and transmission amplitudes are obtained from a pair of simultaneous equations which, when written in matrix notation, define the transfer matrix ... [Pg.150]

Inherent to the optical matrix description of the reflectivity of neutron beams is the assumption that the neutron beam is a wave. Alternatively and entirely equivalently, the neutron could be viewed as a quantum mechnical particle with the reflection process the result of the interaction of the neutron with a potential energy barrier, V. The reflectivity is then the modulus squared of the reflected wave amplitude, the latter quantity being related to the potential energy barrier by the time-independent Schrodinger wave equation. [Pg.69]

Neutrons can also be totally externally reflected when incident at glancing angles. This forms the basis of the technique known as neutron reflectometry (or reflectivity). For a single interface between media i and j the ratio of the reflected and incident amplitudes defines the Fresnel coefficient ... [Pg.86]

From Eq. 1, the evaluation of the characteristic ratio requires measurement of the unperturbed dimensions of the polymer chain. Polymers exhibit their characteristic unperturbed dimensions in the bulk amorphous state, i.e., chain dimensions under these conditions reflect the influence of short range, rotational isomeric state, effects only. Prior to the availability of small-angle neutron scattering (SANS) in the mid-1970s [32-34], no method was available that allowed chain dimensions in polymer melts to be measured directly. SANS utilizes the fact that different isotopes result in different scattering amplitudes for neutrons. Thus, selective deuterium labelling of some chains, followed by dispersing these chains in a solvent of otherwise identical but non-deuterated chains, allows the conformational properties of individual chains to be probed in the melt. [Pg.8]

Box 2 Specular Reflectance and Neutron Wave Field Amplitudes... [Pg.413]


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