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 51
... MaxEnt Reconstruction A 50 100 ( C ) S ( X ) 100 200 300 MaxEnt Reconstruction 50 100 X ( d ) Figure 4 : ( a ) Noisy data resulting from the convolution of the object in Fig . 3 ( a ) with a narrow Gaussian . ( b ) Corresponding data ...
... MaxEnt Reconstruction A 50 100 ( C ) S ( X ) 100 200 300 MaxEnt Reconstruction 50 100 X ( d ) Figure 4 : ( a ) Noisy data resulting from the convolution of the object in Fig . 3 ( a ) with a narrow Gaussian . ( b ) Corresponding data ...
Page 55
... MaxEnt Reconstruction M 50 AA X 100 MaxEnt Reconstruction 50 100 X ( c ) References Day , D.H. & Sinclair , R.N. ( 1969 ) . Neutron Moderator Assemblies for Pulsed Thermal Neutron Time - of - Flight Experiments , Nucl . Instr . Meth ...
... MaxEnt Reconstruction M 50 AA X 100 MaxEnt Reconstruction 50 100 X ( c ) References Day , D.H. & Sinclair , R.N. ( 1969 ) . Neutron Moderator Assemblies for Pulsed Thermal Neutron Time - of - Flight Experiments , Nucl . Instr . Meth ...
Page 230
... MaxEnt reconstruction shown in Fig . 7 ( b ) . This still leaves something to be desired , but is sufficiently close to the truth to provide a good guide towards a suitable functional model . DATA MaxEnt Reconstruction Ref ectivity 0.05 ...
... MaxEnt reconstruction shown in Fig . 7 ( b ) . This still leaves something to be desired , but is sufficiently close to the truth to provide a good guide towards a suitable functional model . DATA MaxEnt Reconstruction Ref ectivity 0.05 ...
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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