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. |
From inside the book
Results 1-3 of 87
Page 254
... shows much improved resolution and some noise suppression over the direct inverse . D ( X ) 5x104 105 O Data 50 X ... shows the Be data for hexamethylene - tetramine ( HMT ) at 15 K taken at the Los Alamos Neutron Scattering Center ...
... shows much improved resolution and some noise suppression over the direct inverse . D ( X ) 5x104 105 O Data 50 X ... shows the Be data for hexamethylene - tetramine ( HMT ) at 15 K taken at the Los Alamos Neutron Scattering Center ...
Page 391
... shows our original germanium analyzer . The original oriented germanium single crystals , of size 4 x 4 x 8 cm were bought from Eagle Picher Industries and hot - pressed in situ on a y - ray diffractometer at the Institut Laue Langevin ...
... shows our original germanium analyzer . The original oriented germanium single crystals , of size 4 x 4 x 8 cm were bought from Eagle Picher Industries and hot - pressed in situ on a y - ray diffractometer at the Institut Laue Langevin ...
Page 678
... shows a simulation analogous to the poisoning of moderators for pulsed neutron sources . Figure 4 ( a ) shows a poisoned R ( x ) ( dashed line ) constructed by convoluting a narrower exponential of 1 / T = 1/2 pixels with the same ...
... shows a simulation analogous to the poisoning of moderators for pulsed neutron sources . Figure 4 ( a ) shows a poisoned R ( x ) ( dashed line ) constructed by convoluting a narrower exponential of 1 / T = 1/2 pixels with the same ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
2 other sections not shown
Other editions - View all
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 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