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Neutron scattering length density profile 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]

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.
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. ...

See other pages where Neutron scattering length density profile calculation is mentioned: [Pg.669]    [Pg.305]    [Pg.248]    [Pg.202]    [Pg.32]    [Pg.278]    [Pg.668]    [Pg.248]    [Pg.445]    [Pg.101]    [Pg.48]   
See also in sourсe #XX -- [ Pg.275 , Pg.277 ]




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