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 101
... inverse Fourier transform in most of the cases . Nonetheless , inverse Fourier transforming remains one of the two approaches in current use . Smoothing or apodization has been used for some time in conjunction with the latter ( Shull ...
... inverse Fourier transform in most of the cases . Nonetheless , inverse Fourier transforming remains one of the two approaches in current use . Smoothing or apodization has been used for some time in conjunction with the latter ( Shull ...
Page 247
... inverse masses to get inverse kinetic energy matrix 1 O 1 G 1 = [ BM 1B ' ] Get symmetry coordinates U Symmetrize G with U to get GU USER r = Bx USER Internal coordinates r Atom positions X Get B USER Get F - matrix from Z - matrix ...
... inverse masses to get inverse kinetic energy matrix 1 O 1 G 1 = [ BM 1B ' ] Get symmetry coordinates U Symmetrize G with U to get GU USER r = Bx USER Internal coordinates r Atom positions X Get B USER Get F - matrix from Z - matrix ...
Page 267
... inverse geometry spectrometer has been a more recent development in comparison with the ToF machines , but it has certain advantages . An inverse geometry spectrometer requires a white incident beam , with the final energy being ...
... inverse geometry spectrometer has been a more recent development in comparison with the ToF machines , but it has certain advantages . An inverse geometry spectrometer requires a white incident beam , with the final energy being ...
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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