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 71
Page 396
... peak should also correspond to zero energy transfer if the calibration is correct . The above procedure was further tested by running with a KBr powder at the sample position using the 220 reflection in Ge for analysing the final energy ...
... peak should also correspond to zero energy transfer if the calibration is correct . The above procedure was further tested by running with a KBr powder at the sample position using the 220 reflection in Ge for analysing the final energy ...
Page 678
... peak intensity , a ten times broader Gaussian R ( x ) produces poorer im- ages than the narrow Gaussian . This provides our first counterexample to this FOM . Next we consider an R ( x ) constructed by convoluting the narrow Gaussian ...
... peak intensity , a ten times broader Gaussian R ( x ) produces poorer im- ages than the narrow Gaussian . This provides our first counterexample to this FOM . Next we consider an R ( x ) constructed by convoluting the narrow Gaussian ...
Page 782
... peak to a steep slope . The tail of the protactinium ( Z = 91 ) peak in the neutron - excess side shrinks and the peak's width becomes wider . The height of the bismuth peak ( Z = 83 ) increases by about one order . Therefore , to ...
... peak to a steep slope . The tail of the protactinium ( Z = 91 ) peak in the neutron - excess side shrinks and the peak's width becomes wider . The height of the bismuth peak ( Z = 83 ) increases by about one order . Therefore , to ...
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