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 99
... injected during an injection period of 375 us . Fig . 3 shows that is nearly proportional to the stored beam intensity . Total losses , L = fĹ dt , will then be quadratic in time . To increase the average current to 100 μA we need to inject ...
... injected during an injection period of 375 us . Fig . 3 shows that is nearly proportional to the stored beam intensity . Total losses , L = fĹ dt , will then be quadratic in time . To increase the average current to 100 μA we need to inject ...
Page 115
... Injection The present method of injection using H ° can be improved using the techniques described above . However , it is much more difficult to improve the H ° beam tune at the foil since it is not possible to focus a neutral beam ...
... Injection The present method of injection using H ° can be improved using the techniques described above . However , it is much more difficult to improve the H ° beam tune at the foil since it is not possible to focus a neutral beam ...
Page 744
... Injection The ring injection takes place via the process H → H + in a 250 - μg / cm2 carbon stripping foil . A plan view of the injection region is shown in Fig . 3 ; the four dipoles in the center translate the proton beam 171.5 mm to ...
... Injection The ring injection takes place via the process H → H + in a 250 - μg / cm2 carbon stripping foil . A plan view of the injection region is shown in Fig . 3 ; the four dipoles in the center translate the proton beam 171.5 mm to ...
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