Advanced Neutron Sources 1988, Proceedings of the 10th Meeting of the INT Collaboration on Advanced Neutron Sources (ICANS X), Held at Los Alamos, October 1988Revolving around the interaction between spectrometer and target-station design and performance, this volume emphasises the need for feedback that must exist between scientific requirements and source design. It achieves a forum for the sharing of information on the development of spallation neutron sources. Of great value to researchers in condensed matter physics, instrumentation and data processing involved in neutron scattering at pulsed and steady sources. |
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Page 358
... count rate in an individual module on SANDALS is unlikely to be sufficient that dead time would be important for ... Count rate calculation and comparison of instruments For liquids and amorphous materials diffraction , irrespective of ...
... count rate in an individual module on SANDALS is unlikely to be sufficient that dead time would be important for ... Count rate calculation and comparison of instruments For liquids and amorphous materials diffraction , irrespective of ...
Page 361
... count rate from a sample of vanadium placed in the neutron beam D4B ( A C Barnes , 1988 , private communication ) . Comparison of this C - number with figure 5 shows that when several angles are combined the LAD diffractometer is ...
... count rate from a sample of vanadium placed in the neutron beam D4B ( A C Barnes , 1988 , private communication ) . Comparison of this C - number with figure 5 shows that when several angles are combined the LAD diffractometer is ...
Page 362
... count rate , isotope substitution diffraction work which is likely to feature very frequently in the SANDALS ... count rates , they will double the resolution in the small angle region . As a further provision the sample tank will ...
... count rate , isotope substitution diffraction work which is likely to feature very frequently in the SANDALS ... count rates , they will double the resolution in the small angle region . As a further provision the sample tank will ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
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accelerator Advanced Neutron Sources analysis angular background beam line Brillouin scattering calculated chopper cold neutron cold source collimators count rate cross section crystal data acquisition deconvolution decoupled density detector deuterium diffraction diffractometer distribution dose effective energy transfer experimental experiments facility factor Figure fission flight path foil function gamma Gaussian geometry high-energy histogram improve increase inelastic injection instrument intensity IPNS irradiation ISIS LAMPF leakage liquid hydrogen Los Alamos magnetic material MaxEnt maximum measured methane module Monte Carlo neutron beam neutron flux neutron scattering Nucl Nuclear obtained operation optimization parameters peak performance Phys position present problems produced proton proton beam radiation radius range reactor reconstruction reflector resolution Rutherford Appleton Laboratory sample scattering angle shield shown in Fig shows solid methane spallation neutron source spallation source spectra spectrometer spectrum surface temperature thermal neutron thick time-of-flight tube wavelength width