## 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 258

A desired

with respect to a particular

physical part of the

...

A desired

**scan**with ROTAX, i.e. the desired rotational function of the motor drivewith respect to a particular

**scan**in the experimentally accessible (Q,«o)-space (physical part of the

**scan**) and its corresponding requirements in the repositioning...

Page 260

In order to improve the

response function has to be performed from time to time. The Fourier transformed

representation of eq. (9) reads: A* = S E* = (A/E) E* = E (10) £ is well known, A is

to be ...

In order to improve the

**scan**performance a deconvolution of the system,sresponse function has to be performed from time to time. The Fourier transformed

representation of eq. (9) reads: A* = S E* = (A/E) E* = E (10) £ is well known, A is

to be ...

Page 261

Invited and Contributed Papers from the Conference on Neutron Scattering Data

Analysis Held at The Rutherford Appleton Laboratory, Chilton, 14-16 March 1990

M. W. Johnson. Fig. 4.

Invited and Contributed Papers from the Conference on Neutron Scattering Data

Analysis Held at The Rutherford Appleton Laboratory, Chilton, 14-16 March 1990

M. W. Johnson. Fig. 4.

**Scan**performance of a a) angular difference "ist"-"soll", ...### What people are saying - Write a review

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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