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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Results 1-3 of 81
Page 345
... measured data . Good agreement between the calculated spectrum and the measured data was obtained , as shown in Fig.2 . This result suggests that the Debye temperature can be well estimated from the effective temperature using Eq . ( 4 ) ...
... measured data . Good agreement between the calculated spectrum and the measured data was obtained , as shown in Fig.2 . This result suggests that the Debye temperature can be well estimated from the effective temperature using Eq . ( 4 ) ...
Page 348
... measured data using only two effective temperatures of Cu and O as parameters . I performed neu- tron absorption ... measured spectra using the effective temperature of Ho as a parameter . Excellent fits to the measured spectra at 300 ...
... measured data using only two effective temperatures of Cu and O as parameters . I performed neu- tron absorption ... measured spectra using the effective temperature of Ho as a parameter . Excellent fits to the measured spectra at 300 ...
Page 778
... measured data [ 3 ] . Both calculated and measured product distributions are in a good agreement in the whole range of N / Z from 1.2 to 1.6 , except in the case of 0.38 - GeV protons . A double- peaked distribution in the curve ...
... measured data [ 3 ] . Both calculated and measured product distributions are in a good agreement in the whole range of N / Z from 1.2 to 1.6 , except in the case of 0.38 - GeV protons . A double- peaked distribution in the curve ...
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