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 140
... line - and accelerator vacuum is necessary . - The material problems for this target version become therefore the prob- lems for the target window- Heat density , Thermal stress Disturbance of material 140 Target materials and engineering.
... line - and accelerator vacuum is necessary . - The material problems for this target version become therefore the prob- lems for the target window- Heat density , Thermal stress Disturbance of material 140 Target materials and engineering.
Page 142
... material distribution and the size of the target . We do not need it here . As a typical example we consider tungsten as target material ( Z = 74 , A = 184 ) and a proton beam energy of 1 GeV . The range of the protons is R ( p ) = 600 ...
... material distribution and the size of the target . We do not need it here . As a typical example we consider tungsten as target material ( Z = 74 , A = 184 ) and a proton beam energy of 1 GeV . The range of the protons is R ( p ) = 600 ...
Page 146
... material in the vicinity should have a lifetime of more then ten years . In order to obtain quantitative information about the behaviour of the ir- radiated material experimental tests of the macroscopic material properties are needed ...
... material in the vicinity should have a lifetime of more then ten years . In order to obtain quantitative information about the behaviour of the ir- radiated material experimental tests of the macroscopic material properties are needed ...
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