## Neutron Scattering Data Analysis 1990: Invited and Contributed Papers from the Conference on Neutron Scattering Data Analysis Held at The Rutherford Appleton Laboratory, Chilton, 14-16 March 1990 |

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Page 138

For the slab can arrangement the strong absorber measurement need not be

presence of the gadolinium mask. When working with slab cans a further

correction is ...

For the slab can arrangement the strong absorber measurement need not be

**performed**as the downstream monitor intensity is always sero due to thepresence of the gadolinium mask. When working with slab cans a further

correction is ...

Page 185

This procedure can be used when it is not possible or it is unlikely to

normalization run. ... In general this operation can be

the spectra obtained from the sample with an independent incoherent spectra

under ...

This procedure can be used when it is not possible or it is unlikely to

**perform**anormalization run. ... In general this operation can be

**performed**by comparingthe spectra obtained from the sample with an independent incoherent spectra

under ...

Page 204

At low Q the Bragg peaks are well separated compared to the resolution width

and thus they are given a weight of zero in the fit

at high Q the Bragg peaks merge together and it becomes impossible to weight ...

At low Q the Bragg peaks are well separated compared to the resolution width

and thus they are given a weight of zero in the fit

**performed**by VANSM. However,at high Q the Bragg peaks merge together and it becomes impossible to weight ...

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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 detector bank determined diffraction data diffractometer distribution function elastic scattering energy error bars example experiment experimental Figure Fourier transform Gaussian GENIE GENIE-V3 histogram inelastic instrument intensity inverse ISIS least squares likelihood function magnetic structure magnetisation density matrix MaxEnt reconstruction Maximum Entropy McGreevy measured method molecular Monte Carlo neutron diffraction neutron scattering normalisation normalization obtained optimisation optimization problems parameters Patterson map performed Phys plot positive powder diffraction presented at Neutron prior procedure quasielastic radial distribution functions refinement reflectivity data resolution function ROTAX Rutherford Appleton Laboratory sample scan scattering law shown simulated annealing single crystal solution spectra spectrometer spectrum statistical structure factor symmetry technique temperature time-of-flight truncation UNIRAS unit cell vanadium vector wavelength workspace