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Neutron scattering length density calculation

Neutron scattering length density profile can be calculated in terms of the known scattering length densities of polymer, pp, and water, p , as... [Pg.275]

It is straightforward to calculate the particle structure facttx from a Fourior transform of the radial distribution of neutron scattering length density, Eq. 2. It is... [Pg.277]

Fig. 2.54 Neutron reflectivity profile for a symmetric PS-dPMMA diblock (Mw 30 kg moP1) as a function of incident wavevector (Russell 1990). The inset shows the scattering length density (b/V, the neutron scattering length per unit volume) profile normal to the film surface that was used to calculate the reflectivity profile shown as the solid line, This is typical of a block copolymer film containing a multilayer stack, with lamellae parallel to the surface. Fig. 2.54 Neutron reflectivity profile for a symmetric PS-dPMMA diblock (Mw 30 kg moP1) as a function of incident wavevector (Russell 1990). The inset shows the scattering length density (b/V, the neutron scattering length per unit volume) profile normal to the film surface that was used to calculate the reflectivity profile shown as the solid line, This is typical of a block copolymer film containing a multilayer stack, with lamellae parallel to the surface.
Fig. 12 Neutron reflectometry (NR) data of the polyelectrolyte multilayer (4 PSS/4 PAH) - coated solid support without lipid bilayer (A), and with a DMPC/DMPG (10 1) mixed membrane on top (C). The curves are shifted relative to each other for clarity. Solid lines represent model calculations of the data with scattering length densities, b/V, corresponding to the blank multilayer support (A), and to the tethered bilayer plus a nonspecific top layer (C), as given in the inset. The dotted line (B) represents a simulation of a lipid bilayer without an additional nonspecific layer on top... Fig. 12 Neutron reflectometry (NR) data of the polyelectrolyte multilayer (4 PSS/4 PAH) - coated solid support without lipid bilayer (A), and with a DMPC/DMPG (10 1) mixed membrane on top (C). The curves are shifted relative to each other for clarity. Solid lines represent model calculations of the data with scattering length densities, b/V, corresponding to the blank multilayer support (A), and to the tethered bilayer plus a nonspecific top layer (C), as given in the inset. The dotted line (B) represents a simulation of a lipid bilayer without an additional nonspecific layer on top...
For calculating the reflection of light it is convenient to use the refractive index and angle of incidence but for neutron reflectivity, it is customary to use scattering length density and momentum transfer. The momentum transfer K is related to the grazing angle of incidence 9 by... [Pg.223]

S A N S can be employed to study both homogeneous as well as heterogenous blends and various information can be derived by analysis of the differential scattering cross-section, d2(Q)/dQ (cm ), where d2(Q) (neutron s ) is the number of neutrons scattered per second into a small solid angle, dQ. The measured intensity, I Q), is related to d 2(Q)/d Q and depends on various parameters such as the incident flux, resolution of the detector, detector efficiency, and so on. It is also a function of the contrast factor (Ag), which is defined as the square of the difference of the scattering length density of the scattering centers, for example, the particle and the matrix. This quantity is calculated from ... [Pg.169]

Figure 5 Left NR profiles for a 523.2 nm film of dPS-ft-PMMA symmetric, diblock copolymer as a function of the neutron momentum normal to the surface at the temperatures indicated. The scattering length density fitl/profiles as a function of depth z, where z= 0 is the air surface, shown in the insets were used to calculate the reflectivity profiles drawn as the solid lines in the figures. Right A log-log plot of the difference between T , and the bulk value of Tout, b as a function of film thickness using the value of Toot, b extrapolated from the NR measurements. Reproduced with permission from Menelle, A. Russell, T. P. Anastasiadis, S. H. etal. Phys. Rev. Lett. 1992, 68,67. ... Figure 5 Left NR profiles for a 523.2 nm film of dPS-ft-PMMA symmetric, diblock copolymer as a function of the neutron momentum normal to the surface at the temperatures indicated. The scattering length density fitl/profiles as a function of depth z, where z= 0 is the air surface, shown in the insets were used to calculate the reflectivity profiles drawn as the solid lines in the figures. Right A log-log plot of the difference between T , and the bulk value of Tout, b as a function of film thickness using the value of Toot, b extrapolated from the NR measurements. Reproduced with permission from Menelle, A. Russell, T. P. Anastasiadis, S. H. etal. Phys. Rev. Lett. 1992, 68,67. ...
Figure 2.59. The electron (left) and nuclear (right) density distributions in the xOz plane of the unit cell of CeRhGcs calculated from x-ray and neutron powder diffraction data, respectively Figure 2.58). The contour of the unit cell is shown schematically as the rectangle under each Fourier map. The peaks correspond to various atoms located in this plane and are so marked on the figure. The volumes of the peaks are proportional to the scattering ability of atoms for x-rays the scattering power decreases in the series Ce(58 e) Rh(45 e) Ge(32 e) for neutrons, the coherent scattering lengths decrease in the reverse order Ge(8.19 fm)... Figure 2.59. The electron (left) and nuclear (right) density distributions in the xOz plane of the unit cell of CeRhGcs calculated from x-ray and neutron powder diffraction data, respectively Figure 2.58). The contour of the unit cell is shown schematically as the rectangle under each Fourier map. The peaks correspond to various atoms located in this plane and are so marked on the figure. The volumes of the peaks are proportional to the scattering ability of atoms for x-rays the scattering power decreases in the series Ce(58 e) Rh(45 e) Ge(32 e) for neutrons, the coherent scattering lengths decrease in the reverse order Ge(8.19 fm)...
Calculate the scattering length and seattering length densities of hydrogenated and perdenterated polystyrene (density = 1.05 g cnr ) and then evaluate the neutron eontrast. [Pg.277]


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Density calculations

Neutron density

Neutron length

Neutron scattering

Neutron scattering length

Neutron scattering length density profile calculation

Neutron-scattering-densities

Neutronic calculation

Neutronics calculations

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Scattering calculations

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