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 263
... accelerator as the preferred device . There are several features of an FFAG accelerator that make it well suited to be the charged - particle accelerator for a 1017 N / cm2 - s pulsed source . Since the main magnets are dc operated ...
... accelerator as the preferred device . There are several features of an FFAG accelerator that make it well suited to be the charged - particle accelerator for a 1017 N / cm2 - s pulsed source . Since the main magnets are dc operated ...
Page 437
... ACCELERATOR POSITION TIME 16 X16 CONTROLS STROBE CONTROLLER HANDSHAKE CAMAC READ GENERATOR POS FIFO 8 16384 x 16 MOD TIME FIFO 16384 x 16 HISTOGRAM ACCELERATOR HANDSHAKE SEGMENT 8 STROBE CAMAC BUS Fig . 7 Block diagram of the Camac ...
... ACCELERATOR POSITION TIME 16 X16 CONTROLS STROBE CONTROLLER HANDSHAKE CAMAC READ GENERATOR POS FIFO 8 16384 x 16 MOD TIME FIFO 16384 x 16 HISTOGRAM ACCELERATOR HANDSHAKE SEGMENT 8 STROBE CAMAC BUS Fig . 7 Block diagram of the Camac ...
Page 439
... Accelerator has completed all required histograming for this event it immediately requests another event from the auxiliary - crate- controller FIFO , so the Histogram Accelerator is the controlling factor in the overall histograming ...
... Accelerator has completed all required histograming for this event it immediately requests another event from the auxiliary - crate- controller FIFO , so the Histogram Accelerator is the controlling factor in the overall histograming ...
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 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