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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Page 239
... Proton Storage Ring Output Beam Parameters Proton Energy 800 MeV Pulse Width Stored protons Instantaneous Current Proton Power Level Neutrons per pulse Total Proton energy 0.27 microseconds 5 X 1013 25 A 30 GW 1015 8 kJ Presently there ...
... Proton Storage Ring Output Beam Parameters Proton Energy 800 MeV Pulse Width Stored protons Instantaneous Current Proton Power Level Neutrons per pulse Total Proton energy 0.27 microseconds 5 X 1013 25 A 30 GW 1015 8 kJ Presently there ...
Page 757
... Proton per MeV into 4π Steradians 10-2 10 " Ep = 2GeV 10-4 10-5 R = 7cm 6cm 5cm 4cm 10- 10-9 10-2 10- ' 10 ° NEUTRON ENERGY ( MEV ) 10 ' 10 ° 10 ' Fig . 5 Leakage neutron spectra from the cylindrical surface of a target for various ...
... Proton per MeV into 4π Steradians 10-2 10 " Ep = 2GeV 10-4 10-5 R = 7cm 6cm 5cm 4cm 10- 10-9 10-2 10- ' 10 ° NEUTRON ENERGY ( MEV ) 10 ' 10 ° 10 ' Fig . 5 Leakage neutron spectra from the cylindrical surface of a target for various ...
Page 803
... proton beam line at a location downstream from where protons are extracted to the White Source experimental area ( see Fig . 1 ) . The 800 - MeV proton beam impinged on a 50 - cm - diam by 200 - cm - long graphite beam stop . The proton ...
... proton beam line at a location downstream from where protons are extracted to the White Source experimental area ( see Fig . 1 ) . The 800 - MeV proton beam impinged on a 50 - cm - diam by 200 - cm - long graphite beam stop . The proton ...
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