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 G [ 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 G [ 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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Common terms and phrases
additional algorithm allows analysis angle applications approach atoms average beam Bragg calculated cell combinatorial optimization configuration constant coordinates correction corresponding cost counts cross-section crystal deconvolution defined density dependent described detector determined diffraction direct display distribution effects elastic scattering energy error estimate example experiment experimental Figure final Fourier function give given inelastic intensity ISIS known limit magnetic Maximum Entropy measured method neutron neutron scattering normalization obtained optimization parameters particular peak performed Phys physical plot positive possible powder presented prior probability problem procedure radial distribution functions range reconstruction References refinement reflections resolution sample scale scan shown shows simulated annealing single solution space spectrum standard statistical structure factor temperature transfer transform unit usually vanadium vector wavelength