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Simulated single crystal diffraction experiment Here D10 is set for a single crystal diffraction experiment in the 4-circle geometry. The polychromatic beam from the thermal neutron guide H24 arrives

CCSL | FullProf | Liquids CCSL CCSL is a library of subroutines for doing crystallographic and related calculations. It is designed not so much as a set of programs for determining and refining struct

First experiment with the 3He neutron spin filter During this first test of an 3 He neutron spin filter, the neutron-beam polarisation transmitted by the filter could be determined with high accuray f

Fig. 1: Cyclic hexamer of adsorbed water in NaXWater molecules (in red) are located on W1 sites. The formation of a cyclic water hexamer in zeolite NaX Neutron powder diffraction is a valuable tool fo

Simulated experiment The polychromatic beam from the hot neutron tube H3 arrives at the monochromator. The monochromatic diffracted beam reaches the sample – a single crystal - located at the centre o

(png - 227 Ki) A 3D layout of CYCLOPS showing how the 16 CCD detectors are distributed around the sample. CYCLOPS - Neutron Laue single-crystal diffractometer CYCLOPS (CYlindrical Ccd Laue Octagonal P

Density dependence of collective modes in molten Rubidium Understanding the density dependence of collective dynamics in liquid metals is still a difficult task since the interatomic interactions are

Caption Fig.1. Dynamic structure factor of gold at four Q values of the NBS experiment performed on BRISP. The experimental data (black dots) are broadened by the instrumental energy resolution. The c

(jpg - 82 Ki) Caption Fig.1: Dispersion relations for molten RbBr. Triangles are the ωl values from the S(Q, ω), and circles are the peak values from the current spectra J (Q,ω). The line with dots is

(png - 569 Ki) Caption Fig.1: Dynamic structure factor of liquid gold at five Q values measured on BRISP. The experimental data (blue dots) are broadened by the instrumental energy resolution. The RJ-