Neutron Scattering Data Analysis 1990, Proceedings of the Conference on Neutron Scattering, 14-16 March 1990, Rutherford Appleton Laboratory, UKM. W. Johnson |
From inside the book
Results 1-3 of 51
Page 99
... intensities for TiO2 ME Map Origin Peak X y Z Δ ME intensity True intensity 0.0000 0.0000 0.0000 0.0000 1.671 1.147 Ti - O 0.3041 0.3041 0.0000 0.0010 -0.387 -0.399 O - O 0.3949 0.3949 0.0000 0.0064 0.325 0.337 Ti - Ti 0.5000 0.5000 ...
... intensities for TiO2 ME Map Origin Peak X y Z Δ ME intensity True intensity 0.0000 0.0000 0.0000 0.0000 1.671 1.147 Ti - O 0.3041 0.3041 0.0000 0.0010 -0.387 -0.399 O - O 0.3949 0.3949 0.0000 0.0064 0.325 0.337 Ti - Ti 0.5000 0.5000 ...
Page 138
... 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 where μ varies with wavelength the ...
... 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 where μ varies with wavelength the ...
Page 143
... intensity . However , the presence of a contaminant material cannot explain why the final corrected intensity from the vanadium in the furnace increases at longer wavelengths relative to the non - furnace vanadium intensity . This ...
... intensity . However , the presence of a contaminant material cannot explain why the final corrected intensity from the vanadium in the furnace increases at longer wavelengths relative to the non - furnace vanadium intensity . This ...
Other editions - View all
Common terms and phrases
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