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
... sample in the sample can , an empty sample can , and a sample can filled with a strong absorber such as B4C . For the slab can arrangement the strong absorber measurement need not be performed as the downstream monitor intensity is ...
... sample in the sample can , an empty sample can , and a sample can filled with a strong absorber such as B4C . For the slab can arrangement the strong absorber measurement need not be performed as the downstream monitor intensity is ...
Page 140
... sample absorption was considerable for both volumes of sample ; for the 15mm thick sample μD varied from 0.7 to 1.7 over the measured wavelength range of 0.5 to 4.5Å . As the effective absorption of KH , PO is not known we were unable ...
... sample absorption was considerable for both volumes of sample ; for the 15mm thick sample μD varied from 0.7 to 1.7 over the measured wavelength range of 0.5 to 4.5Å . As the effective absorption of KH , PO is not known we were unable ...
Page 141
... sample mass for a CrOOH sample in a 5mm thick slab sample can . Shown on the same scale but shifted by 100 intensity units is the difference between the absorption corrected intensity divided by sample mass for a 5mm and a 15mm thick sample ...
... sample mass for a CrOOH sample in a 5mm thick slab sample can . Shown on the same scale but shifted by 100 intensity units is the difference between the absorption corrected intensity divided by sample mass for a 5mm and a 15mm thick sample ...
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Acta Cryst algorithm applications approach atoms Bayesian beam Bragg peaks calculated configuration constraints coordinates corresponding cost function cross-section crystallographic Data Anal data analysis data set defined determined diffraction data diffractometer distribution elastic scattering energy error bars example experiment experimental Figure Fourier transform Gaussian GENIE GENIE-V3 histogram inelastic instrument intensity interpolation inverse ISIS likelihood function magnetic structure Markov chain matrix MaxEnt Reconstruction Maximum Entropy McGreevy measured method molecular MoO3 neutron diffraction neutron scattering normalisation normalization obtained optimisation optimization problems parameters Patterson map performed Phys plot positive powder diffraction presented at Neutron prior probability procedure quasielastic refinement reflectivity data resolution function ROTAX Rutherford Appleton Laboratory sample scan Scatt scattering law shown simulated annealing single crystal solution spectra spectrometer spectrum statistical structure factor symmetry temperature time-of-flight truncation UNIRAS unit cell vanadium vector wavelength workspace