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 74
... vector . Time chan- nels or data values may be modelled as vectors . Vectors in general may have any length , GENIE - V3 imposes no pre - defined length on vectors . Some operations though may require two vectors to be of identical ...
... vector . Time chan- nels or data values may be modelled as vectors . Vectors in general may have any length , GENIE - V3 imposes no pre - defined length on vectors . Some operations though may require two vectors to be of identical ...
Page 75
... VECTOR The concept can be further extended upwards by modelling the entity " Histogram " which makes use of two ... vector Integer vector String vector Workspace Workspace vector Detector map 2 - D Histogram External views of GENIE ...
... VECTOR The concept can be further extended upwards by modelling the entity " Histogram " which makes use of two ... vector Integer vector String vector Workspace Workspace vector Detector map 2 - D Histogram External views of GENIE ...
Page 98
... vector peaks caused by misapportioning of Bragg intensities . It is not possible to locate the interatomic vectors ( listed in Table 1 ) with any degree of confidence . Using a uniform prior distribution , a maximum Patterson map con ...
... vector peaks caused by misapportioning of Bragg intensities . It is not possible to locate the interatomic vectors ( listed in Table 1 ) with any degree of confidence . Using a uniform prior distribution , a maximum Patterson map con ...
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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