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 126
... gamma - ray flux than neutron flux to produce 1 mrem / hr . Thus , the energies of neutrons and gamma rays leaking through a shield can have profound effects on the total dose at the shield surface . The rapid change of the flux - to ...
... gamma - ray flux than neutron flux to produce 1 mrem / hr . Thus , the energies of neutrons and gamma rays leaking through a shield can have profound effects on the total dose at the shield surface . The rapid change of the flux - to ...
Page 127
... gamma rays ) at the shield surface . Detectors also respond to both neutrons and gamma - rays , therefore , gamma rays must be accounted for when designing detector shielding . All low - energy neutrons that do not undergo particle ...
... gamma rays ) at the shield surface . Detectors also respond to both neutrons and gamma - rays , therefore , gamma rays must be accounted for when designing detector shielding . All low - energy neutrons that do not undergo particle ...
Page 128
... gamma rays , we mean those gamma rays produced by high - energy reactions . Secondary low - energy gamma rays result from secondary low - energy neutron interactions . These two gamma - ray components sum to give a segment we call ...
... gamma rays , we mean those gamma rays produced by high - energy reactions . Secondary low - energy gamma rays result from secondary low - energy neutron interactions . These two gamma - ray components sum to give a segment we call ...
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