Neutron ScatteringG. Kostorz |
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Page 79
... detector ( 5 mm ) . It is not possible to use collimators or slit systems between the sample and the detector which means that scattering from all material in the sample region will enter the detector ; great efforts are therefore made ...
... detector ( 5 mm ) . It is not possible to use collimators or slit systems between the sample and the detector which means that scattering from all material in the sample region will enter the detector ; great efforts are therefore made ...
Page 83
... detector and crystal should be scanned through the nominal reflecting position with the detector moving through twice the angle of the crystal ( 0 – 20 scan ) . The other extreme case is when the angular divergence of the beam plus the ...
... detector and crystal should be scanned through the nominal reflecting position with the detector moving through twice the angle of the crystal ( 0 – 20 scan ) . The other extreme case is when the angular divergence of the beam plus the ...
Page 253
... detector tube ( see Fig . 6 ) . The collimation and detector tubes are each about 40 m long , and to fixed detector positions of 2.5 , 5.5 , 10.5 , 20.5 , 40.5 m from the small sample vessel , there are corresponding pieces of straight ...
... detector tube ( see Fig . 6 ) . The collimation and detector tubes are each about 40 m long , and to fixed detector positions of 2.5 , 5.5 , 10.5 , 20.5 , 40.5 m from the small sample vessel , there are corresponding pieces of straight ...
Contents
Neutron Production and Detection | 12 |
Basic Scattering Theory | 21 |
Diffraction from Crystals | 30 |
Copyright | |
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Other editions - View all
Neutron Scattering: Treatise on Materials Science and Technology, Volume 15 G. Kostorz Limited preview - 2013 |
Common terms and phrases
alloys amplitude antiferromagnetic atoms average Bragg peaks Bragg scattering calculated chain chapter by Kostorz Chem coherent collimation concentration cross section Crystallogr Debye-Waller factor defect density dependence detector direction dispersion curves displacements distribution domain elastic electron energy experimental ferroelectric ferromagnetic flux line frequency hydrides hydrogen impurity incoherent scattering inelastic scattering Institut Laue-Langevin intensity interaction isotope Kostorz and Lovesey Lett magnetic scattering materials matrix measurements metal mode molecules monochromator neutron beam neutron diffraction neutron SAS neutron scattering nuclear obtained orientation parameters particles peak phase phonon Phys plane polarized neutron polymer Proc quasi-elastic reactor reciprocal lattice reflection resolution sample scattering cross section scattering length scattering vector Schelten Schmatz shown in Fig single crystal solid spin structure factor studies symmetry technique temperature theory thermal neutron tion transition unit cell values wave vector wavelength width x-ray ΦΩ
References to this book
Einführung in die Kristallographie Will Kleber,Hans-Joachim Bautsch,Joachim Bohm No preview available - 1998 |