Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01978003906064500

It has three components: i an array of positive charges situated at the positions of the surface atom nuclei, each charge being of a size necessary to satisfy the Gauss result: ii

given by the entrance windows of the beam tube and f o r short wavelength by the curvature of the following guide.. This leads t o a flux dilution factor which varies over the height of

We note that this is very similar to the values obtained from second virial coefficient measurements of Ar by Wolfe and Sams [35] ; ii dislocations influence the form of the

The fact that both Dy and Ni can be obtained with a zero scattering length also means that it is possible to prepare a sample for whlch the nuclear scattering is compietely incoherent

The explanation is that on the one hand new reflection peaks due to the intermediate phases are too small to be seen the measurement on single crystal are much more sensitive than the

- Total pair distribution functions for the measured samples as obtained by direct Fourier transformation of the structure factors shown in figure 4.. Partial pair distribution

2014 This work gives an explanation of the anomalous neutron diffraction effect on 03B1-LiIO3 based on elastic dipole theory and shows that by analysing the dynamical processes one can

DYNAMICAL EFFECTS IN NEUTRON OPTICS AND SPIN INTERACTIONS M... To evaluate the flux