Neutron ScatteringG. Kostorz |
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Page 13
... reactor ( PIK ) currently under construction will have a higher flux than any existing steady - state reactor , and more thermal neutrons will be extracted by larger beam tubes . ] The High Flux Beam Reactor at Brookhaven National ...
... reactor ( PIK ) currently under construction will have a higher flux than any existing steady - state reactor , and more thermal neutrons will be extracted by larger beam tubes . ] The High Flux Beam Reactor at Brookhaven National ...
Page 16
... reactor beam tubes cannot exceed a diameter of about 30 cm and have a minimum length of 3-4 m . At ILL they are typically 4-5 m long and have a maximum beam cross section of 15 x 15 cm2 . The useful flux at the beam tube exit is thus ...
... reactor beam tubes cannot exceed a diameter of about 30 cm and have a minimum length of 3-4 m . At ILL they are typically 4-5 m long and have a maximum beam cross section of 15 x 15 cm2 . The useful flux at the beam tube exit is thus ...
Page 18
... reactor IBR - 1 at Dubna ( USSR ) ( see Cocking and Webb , 1965 ) , now known as IBR 30 , with a peak thermal flux of about 3 x 1014 / cm2 sec . A new pulsed reactor , IBR - 2 , is currently under construction and will produce a peak ...
... reactor IBR - 1 at Dubna ( USSR ) ( see Cocking and Webb , 1965 ) , now known as IBR 30 , with a peak thermal flux of about 3 x 1014 / cm2 sec . A new pulsed reactor , IBR - 2 , is currently under construction and will produce a peak ...
Contents
Neutron Production and Detection | 12 |
Basic Scattering Theory | 21 |
Diffraction from Crystals | 30 |
Copyright | |
18 other sections not shown
Other editions - View all
Neutron Scattering: Treatise on Materials Science and Technology, Volume 15 G. Kostorz Limited preview - 2013 |
Common terms and phrases
alloys angle application atoms average beam Bragg calculated cell chapter coherent concentration constant containing contributions corresponding cross section crystal curves defect defined density dependence described detailed detector determined diffraction diffuse direction discussed displacements distribution domain effects elastic elastic scattering electron energy et al example experimental experiments factor field flux forces frequency function give given hydrogen important incident incoherent indicate inelastic intensity interaction Kostorz lattice limit Lovesey magnetic materials means measurements metal method mode monochromator neutron diffraction neutron scattering nuclear observed obtained orientation parameters peak phase phonon Phys plane polarization polymer positions possible properties range recent reflection relative resolution sample shown shows simple solid solution space structure studies technique temperature theory thermal tion transition unit values vector volume wave wavelength width x-ray
References to this book
Einführung in die Kristallographie Will Kleber,Hans-Joachim Bautsch,Joachim Bohm No preview available - 1998 |