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 119
... present BPM's are also of limited use for studying broad - band phenomena such as the trans- verse instability . A program of BPM development is underway to develop instruments that satisfy these needs . Knowledge of the distribution of ...
... present BPM's are also of limited use for studying broad - band phenomena such as the trans- verse instability . A program of BPM development is underway to develop instruments that satisfy these needs . Knowledge of the distribution of ...
Page 791
... Present results are very much different from those by Bauer , et al . We confirmed TN ~ 33K , while they reported a value of TN ~ 80K . The present results show that the increase of the gain comes mainly from the coupling with reflector ...
... Present results are very much different from those by Bauer , et al . We confirmed TN ~ 33K , while they reported a value of TN ~ 80K . The present results show that the increase of the gain comes mainly from the coupling with reflector ...
Page 795
... present values , however , are considerably larger than those of the KENS solid methane moderator . Neutron pulse widths , in full width at half maximum ( FWHM ) , from these two moderators are plotted in Fig . 10 as a function of ...
... present values , however , are considerably larger than those of the KENS solid methane moderator . Neutron pulse widths , in full width at half maximum ( FWHM ) , from these two moderators are plotted in Fig . 10 as a function of ...
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