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 90
Page 19
... range 10-500 meV 1 % energy transfer resolution - 3-135 ° . ho range 2-1500 meV - 1.5 % energy transfer resolution , elastic line width 0.2 meV . Graphite analyser ( 002 ) reflection : 15 peV resolution at 1.83 meV E a Qa- 0.25-1.85 A ...
... range 10-500 meV 1 % energy transfer resolution - 3-135 ° . ho range 2-1500 meV - 1.5 % energy transfer resolution , elastic line width 0.2 meV . Graphite analyser ( 002 ) reflection : 15 peV resolution at 1.83 meV E a Qa- 0.25-1.85 A ...
Page 235
... range . The rising cross section of hydrogen as the energy decreases into the thermal range improves the polarization substantially above the eV range value of about 55 % . However the transmission of the neutrons decreases rapidly as ...
... range . The rising cross section of hydrogen as the energy decreases into the thermal range improves the polarization substantially above the eV range value of about 55 % . However the transmission of the neutrons decreases rapidly as ...
Page 282
... range is required . At full ISIS frequency the wavelength window at the sample is 2.0 Å . The energy transfer range spanned depends upon the phase of the chopper with respect to the ISIS pulse . If the wavelength window is centred on ...
... range is required . At full ISIS frequency the wavelength window at the sample is 2.0 Å . The energy transfer range spanned depends upon the phase of the chopper with respect to the ISIS pulse . If the wavelength window is centred on ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
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Common terms and phrases
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