## 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 72

It is quite easy to see how the entity being modelled "a one- dimensional

Unfortunately, because the structure of the code in GENIE- V2 does not model

the ...

It is quite easy to see how the entity being modelled "a one- dimensional

**histogram**" can be generalized to "a two-dimensional**histogram**" (see Figure 2).Unfortunately, because the structure of the code in GENIE- V2 does not model

the ...

Page 78

The obvious omissions from this list are types like "

spectrum." The type "Workspace" also implies that GENTE-V3 is modelling some

physical entity called a workspace which has not yet been mentioned. 5.2

Workspaces ...

The obvious omissions from this list are types like "

**Histogram**" and "TOFspectrum." The type "Workspace" also implies that GENTE-V3 is modelling some

physical entity called a workspace which has not yet been mentioned. 5.2

Workspaces ...

Page 88

The plot in Figure 5d is a

through the centre. It clearly shows that the two peaks are not the same height

and there are possible shoulders on their sides which may be physically

significant.

The plot in Figure 5d is a

**histogram**of the values in the data along the linethrough the centre. It clearly shows that the two peaks are not the same height

and there are possible shoulders on their sides which may be physically

significant.

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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 detector bank determined diffraction data diffractometer elastic scattering energy error bars example experiment experimental Figure Fourier transform Gaussian GENIE GENIE-V3 histogram inelastic instrument intensity interpolation inverse ISIS least squares likelihood function magnetic structure magnetisation density Markov chain 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 probability procedure quasielastic 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 UNIRAS unit cell vanadium vector wavelength workspace