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. |
From inside the book
Results 1-3 of 81
Page 215
... maximum value of the ratio obtained is slightly less than 1.5 and is for the highest energy group shown that is group 4. For group 5 , the maximum value obtained is considerably smaller ; for group 6 , the maximum value obtained is ...
... maximum value of the ratio obtained is slightly less than 1.5 and is for the highest energy group shown that is group 4. For group 5 , the maximum value obtained is considerably smaller ; for group 6 , the maximum value obtained is ...
Page 434
... Maximum instantaneous data rate per detector Maximum time - averaged data rate per detector Maximum number of detector elements 64 elements / detector ~ 2 5x104 n / sec / det 1x103 n / sec / det 450 detectors ~ 29,000 elements ~ 4.5x105 ...
... Maximum instantaneous data rate per detector Maximum time - averaged data rate per detector Maximum number of detector elements 64 elements / detector ~ 2 5x104 n / sec / det 1x103 n / sec / det 450 detectors ~ 29,000 elements ~ 4.5x105 ...
Page 736
... maximum entropy and Bayesian methods . Bayes ' theorem pro- vides a systematic approach to statistical inference . It states that the prob- ability of the image after an experiment ( the Posterior ) is the product of the probability of ...
... maximum entropy and Bayesian methods . Bayes ' theorem pro- vides a systematic approach to statistical inference . It states that the prob- ability of the image after an experiment ( the Posterior ) is the product of the probability of ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
2 other sections not shown
Other editions - View all
Common terms and phrases
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 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