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 686
... spectrum is broadened by the resolution function and noise ( with Poisson statistics ) is added to produce the observed spectrum . The METRIC [ 4 ] MaxEnt method is then used to deconvolute the observed spectrum using the broadening ...
... spectrum is broadened by the resolution function and noise ( with Poisson statistics ) is added to produce the observed spectrum . The METRIC [ 4 ] MaxEnt method is then used to deconvolute the observed spectrum using the broadening ...
Page 855
... spectrum value to be used for personnel dosimetry records . Introduction On July 22 , 1987 an experiment was run to measure the neutron energy spectrum in the LANSCE Experiment Room 1 ( ER - 1 ) with the proton beam being stopped in the ...
... spectrum value to be used for personnel dosimetry records . Introduction On July 22 , 1987 an experiment was run to measure the neutron energy spectrum in the LANSCE Experiment Room 1 ( ER - 1 ) with the proton beam being stopped in the ...
Page 857
... spectrum determined from the unfolding codes is shown in Fig . 2. The codes show good general agreement up to about 60 MeV . There is poorer agreement in the number of neutrons present above that energy . The neutron - radiation field ...
... spectrum determined from the unfolding codes is shown in Fig . 2. The codes show good general agreement up to about 60 MeV . There is poorer agreement in the number of neutrons present above that energy . The neutron - radiation field ...
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