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 83
Page 332
... function , as has been previously discussed [ 4 ] . For the two - slot two chopper system the function is unity for < x - 1 , where = - V ( St1 - St2 ) / 4b and x = B / 2b , and otherwise it is zero . For the four - slot three chopper ...
... function , as has been previously discussed [ 4 ] . For the two - slot two chopper system the function is unity for < x - 1 , where = - V ( St1 - St2 ) / 4b and x = B / 2b , and otherwise it is zero . For the four - slot three chopper ...
Page 664
... function and maintaining the three parameters described above , a scale factor , and a delay time to , as free parameters of wavelength . The results of the fitting , while encouraging , were not spectacular . Fig . 5 shows the results ...
... function and maintaining the three parameters described above , a scale factor , and a delay time to , as free parameters of wavelength . The results of the fitting , while encouraging , were not spectacular . Fig . 5 shows the results ...
Page 699
... functions . In Figures 13-17 , A is the observed data , B is the resulting deconvolution , C is the resolution function and D is the intrinsic spectrum . Fig . No. of Peaks Sep. Broadening ( us ) FWHM . FWHMY Function 13 1 3.0 17.0 ...
... functions . In Figures 13-17 , A is the observed data , B is the resulting deconvolution , C is the resolution function and D is the intrinsic spectrum . Fig . No. of Peaks Sep. Broadening ( us ) FWHM . FWHMY Function 13 1 3.0 17.0 ...
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 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