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 327
... intensity transmitted by multiple - slot multiple disk chopper systems J. R. D. Copley University of Maryland College Park , Maryland 20742 and National Institute of Standards and Technology Gaithersburg , Maryland 20899 USA ABSTRACT ...
... intensity transmitted by multiple - slot multiple disk chopper systems J. R. D. Copley University of Maryland College Park , Maryland 20742 and National Institute of Standards and Technology Gaithersburg , Maryland 20899 USA ABSTRACT ...
Page 333
... intensity significantly , but little intensity appears in the satellites if it is turned off . For example , the integrated intensity ratio Ip ( o ) / Ip ( 0 ) is reduced from ~ 0.99 to 0.83 when σ = 1 μs ( ~ 0.97 to 0.53 when σ = 2 μs ) ...
... intensity significantly , but little intensity appears in the satellites if it is turned off . For example , the integrated intensity ratio Ip ( o ) / Ip ( 0 ) is reduced from ~ 0.99 to 0.83 when σ = 1 μs ( ~ 0.97 to 0.53 when σ = 2 μs ) ...
Page 612
... intensity , making the utmost of our low repetition rate and high pulse intensity , and instruments that work in the extremes of the energy range - in particular , the higher energies . Not only would we be able to do experiments that ...
... intensity , making the utmost of our low repetition rate and high pulse intensity , and instruments that work in the extremes of the energy range - in particular , the higher energies . Not only would we be able to do experiments that ...
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