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 5
... matrix . The matrix C should be faithful to our underlying prior ideas about the configuration space x on which it operates . Being part of our prior model , it is to be independent of the particular points { x } which will ( later ) be ...
... matrix . The matrix C should be faithful to our underlying prior ideas about the configuration space x on which it operates . Being part of our prior model , it is to be independent of the particular points { x } which will ( later ) be ...
Page 216
... matrix per layer in terms of Fresnel coefficients and phase factors , derived in optical terms from the relationship between electric vectors in successive layers . A characteristic matrix per layer ( analogous to that defined in ...
... matrix per layer in terms of Fresnel coefficients and phase factors , derived in optical terms from the relationship between electric vectors in successive layers . A characteristic matrix per layer ( analogous to that defined in ...
Page 247
... 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 Diagonalize GU to getW and diagonal elemets DG ...
... 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 Diagonalize GU to getW and diagonal elemets DG ...
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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