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 36
... chopper , optimized for transmission of 10 meV neutrons , has been fabricated and tested . Unfortunately , this ... system is being designed to operate the Fermi choppers and the to choppers . This system will implement the same ...
... chopper , optimized for transmission of 10 meV neutrons , has been fabricated and tested . Unfortunately , this ... system is being designed to operate the Fermi choppers and the to choppers . This system will implement the same ...
Page 303
... System 3.1 . Monochromating Chopper and Background Suppression Chopper A chopper system is supplied from RAL as a part of the UK - Japan collaboration . The chopper is equipped with a magnetic bearing system developed at KFA , Jülich6 ) .
... System 3.1 . Monochromating Chopper and Background Suppression Chopper A chopper system is supplied from RAL as a part of the UK - Japan collaboration . The chopper is equipped with a magnetic bearing system developed at KFA , Jülich6 ) .
Page 332
... choppers should be continuously monitored , and contaminated pulses should be rejected by the data acquisition system . Similar considerations apply to the case of the three chopper system illustrated in Fig . 1 ( d ) . The rejection of ...
... choppers should be continuously monitored , and contaminated pulses should be rejected by the data acquisition system . Similar considerations apply to the case of the three chopper system illustrated in Fig . 1 ( d ) . The rejection of ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
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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 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