Pulsed Neutron Scattering |
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Page 75
... Accelerator Static Booster ( ii ) Dynamic Booster Fissile or Reflecting Rotor ( iii ) Reactivity Reactivity O O Time Time Time Figure 2.5 . Pulsed neutron sources using fission . ( i ) In the pulsed reactor , the reactivity of the core ...
... Accelerator Static Booster ( ii ) Dynamic Booster Fissile or Reflecting Rotor ( iii ) Reactivity Reactivity O O Time Time Time Figure 2.5 . Pulsed neutron sources using fission . ( i ) In the pulsed reactor , the reactivity of the core ...
Page 84
... accelerator walls can be damaged . What determines the final current in a proton synchrotron ? There is no easy answer to this a fact which explains the widely differing calculated perfor- mances of apparently similar accelerators ...
... accelerator walls can be damaged . What determines the final current in a proton synchrotron ? There is no easy answer to this a fact which explains the widely differing calculated perfor- mances of apparently similar accelerators ...
Page 88
... accelerator installation76 . Phase I , due for completion in 1981 , uses the spare protons from the 500 MeV injector accelerator of the zero gradient synchrotron ( ZGS ) . Phase II comprises a new accelerator , making use of facilities ...
... accelerator installation76 . Phase I , due for completion in 1981 , uses the spare protons from the 500 MeV injector accelerator of the zero gradient synchrotron ( ZGS ) . Phase II comprises a new accelerator , making use of facilities ...
Common terms and phrases
absorption accelerator atoms background beam tube beryllium Bragg reflection calculated cell collimation count-rate counter bank cross-section crystal monochromator curve defined density depends detector diffraction diffractometer direct geometry distribution dose E₁ effective efficiency elastic electron linac energy transfer epithermal equation fast neutrons figure of merit fission function given gives Harwell hydrogen incident beam incident energy incident flight path incident neutron intensity k₁ L₁ linac magnetic Maxwellian measured neutron beam neutron scattering neutron source nuclear nuclei phonon polarization proton pulse width pulsed neutron pulsed reactor pulsed source Q values Qmax radiation range ratio reciprocal lattice reciprocal space reflector resolution element resonance rotor sample scattered flight path scattering angle scattering length scattering vector Section shielding shown in figure shows single crystal slit solid angle spallation spectrometer spectrum spin target thermal thickness time-of-flight transmission typical vanadium velocity vibrational wave-vector wavelength y-rays Δι ΦΩ
References to this book
Polymers and Neutron Scattering Julia S. Higgins,Henri C. Benoît,Henri Benoît No preview available - 1996 |