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 141
... density , Thermal stress Disturbance of material properties by radiation Compatibility between liquid and solid metal Macro - Cyclic Stress We recognize that for each target version quite specific difficulties have to be overcome . On ...
... density , Thermal stress Disturbance of material properties by radiation Compatibility between liquid and solid metal Macro - Cyclic Stress We recognize that for each target version quite specific difficulties have to be overcome . On ...
Page 143
... density , then for high total power ii ) For a spallation source we essentially aim for high beam power . De- creasing the target size would increase the power density on a window like pu ~ P The Problem of Power Density As general ...
... density , then for high total power ii ) For a spallation source we essentially aim for high beam power . De- creasing the target size would increase the power density on a window like pu ~ P The Problem of Power Density As general ...
Page 144
... density of 4004 from the proton beam . The power density in a stationary target - window or - plate becomes larger then 20MW . Hence a moving target including target - window seems to be unavoidable . ст We admit that for a pulsed ...
... density of 4004 from the proton beam . The power density in a stationary target - window or - plate becomes larger then 20MW . Hence a moving target including target - window seems to be unavoidable . ст We admit that for a pulsed ...
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