Elements of X-ray DiffractionIntended to acquaint the reader with the theory of x-ray diffraction, the experimental methods involved, and the main applications. The book is a collection of principles and methods stressing X-ray diffraction rather than metallurgy. KEY TOPICS: The book is written entirely in terms of the Bragg law and can be read without any knowledge of the reciprocal lattice. It is divided into three main parts--Fundamentals; experimental methods; and applications. MARKET: Designed for beginners, not as a reference tool for the advanced reader. |
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Page 128
... electrons ? More precisely , does an atom of atomic number Z , i.e. , an atom containing Z electrons , scatter a wave whose amplitude is Z times the amplitude of the wave scattered by a single electron ? The answer is yes , if the ...
... electrons ? More precisely , does an atom of atomic number Z , i.e. , an atom containing Z electrons , scatter a wave whose amplitude is Z times the amplitude of the wave scattered by a single electron ? The answer is yes , if the ...
Page 575
... electron . The closer the electrons are to the optic axis , the smaller their deflection , and electrons traveling exactly on the optic axis experience no deflection . Note that the electrons off the plane shown and off the optic axis ...
... electron . The closer the electrons are to the optic axis , the smaller their deflection , and electrons traveling exactly on the optic axis experience no deflection . Note that the electrons off the plane shown and off the optic axis ...
Page 616
... electrons also supplies crystallographic information and has received increasing attention recently . Electron diffraction is therefore well suited to the study of thin surface layers . 2 . Electrons are scattered much more intensely ...
... electrons also supplies crystallographic information and has received increasing attention recently . Electron diffraction is therefore well suited to the study of thin surface layers . 2 . Electrons are scattered much more intensely ...
Contents
Geometry of Crystals | 31 |
Geometry | 89 |
Intensities Diffraction | 123 |
Copyright | |
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absorption alloy angle appear applied atoms axis calculated called camera cause circle complete consider constant contains counting crystal cubic curve depends described detector determined diffracted beam diffraction lines diffraction pattern diffractometer direction distance effect electrons energy equal equation error example factor Figure film fraction function given grain hexagonal incident beam increases indices intensity kind lattice Laue material means measured metal method normal Note observed obtained occur orientation origin parallel parameter particular pattern peak percent phase plane plot pole position possible powder produce projection radiation rays reciprocal lattice recorded reference reflection region relation relative result rotation sample scattering shown shown in Fig shows simple single solid space specimen sphere stress structure surface temperature tion transmission tube unit cell usually vector wave wavelength x-ray