Neutron Scattering Data Analysis 1990, Proceedings of the Conference on Neutron Scattering, 14-16 March 1990, Rutherford Appleton Laboratory, UKM. W. Johnson |
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Page 138
... performed as the downstream monitor intensity is always zero due to the presence of the gadolinium mask . When working with slab cans a further correction is sometimes necessary due to the presence of the gadolinium mask . For a sample ...
... performed as the downstream monitor intensity is always zero due to the presence of the gadolinium mask . When working with slab cans a further correction is sometimes necessary due to the presence of the gadolinium mask . For a sample ...
Page 204
... performed by VANSM . However , at high Q the Bragg peaks merge together and it becomes impossible to weight them out . The second reason for performing a fit is to filter out noise since ( excluding the Bragg peaks ) vanadium gives rise ...
... performed by VANSM . However , at high Q the Bragg peaks merge together and it becomes impossible to weight them out . The second reason for performing a fit is to filter out noise since ( excluding the Bragg peaks ) vanadium gives rise ...
Page 243
... performing regrouping by software , following the experiment . This enabled us to identify a number of artefacts which may be ascribed to the planar geometry of the detector . This has additional implications in experiments performed at ...
... performing regrouping by software , following the experiment . This enabled us to identify a number of artefacts which may be ascribed to the planar geometry of the detector . This has additional implications in experiments performed at ...
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Common terms and phrases
additional algorithm allows analysis angle applications approach atoms average beam Bragg calculated cell combinatorial optimization configuration constant coordinates correction corresponding cost counts cross-section crystal deconvolution defined density dependent described detector determined diffraction direct display distribution effects elastic scattering energy error estimate example experiment experimental Figure final Fourier function give given inelastic intensity ISIS known limit magnetic Maximum Entropy measured method neutron neutron scattering normalization obtained optimization parameters particular peak performed Phys physical plot positive possible powder presented prior probability problem procedure radial distribution functions range reconstruction References refinement reflections resolution sample scale scan shown shows simulated annealing single solution space spectrum standard statistical structure factor temperature transfer transform unit usually vanadium vector wavelength