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 77
Page 381
... scattering [ 8 ] or inelastic effects [ 3 ] , may also be seen from such plots . Future directions The basic ... Neutron Scattering " , Nucl . Instr . Meth . , A245 , 115-124 . 2. Hjelm , R.P. , Jr. , 1987 , " Resolution of Time - of - Flight ...
... scattering [ 8 ] or inelastic effects [ 3 ] , may also be seen from such plots . Future directions The basic ... Neutron Scattering " , Nucl . Instr . Meth . , A245 , 115-124 . 2. Hjelm , R.P. , Jr. , 1987 , " Resolution of Time - of - Flight ...
Page 674
... neutron scattering law , S ( x ) , from the data , D ( x ) . In a representative neutron scattering experiment , the neutron scattering law , S ( x ) , we wish to measure may be as shown in Fig . 1 ( a ) . As a first approxi- mation R ...
... neutron scattering law , S ( x ) , from the data , D ( x ) . In a representative neutron scattering experiment , the neutron scattering law , S ( x ) , we wish to measure may be as shown in Fig . 1 ( a ) . As a first approxi- mation R ...
Page 735
... neutron scatter- ing law , which is proportional to the correlation functions of the condensed matter systems of scientific interest . The data produced in neutron scattering experiments is equal to a convolution of the scattering law ...
... neutron scatter- ing law , which is proportional to the correlation functions of the condensed matter systems of scientific interest . The data produced in neutron scattering experiments is equal to a convolution of the scattering law ...
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 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