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 214
... peak may be misleading to some . Note that the size of escape - peak pulses corresponds not to the escaping energy , but to the difference between the normal and escaping energies . ) Shown in ( b ) are the normal and escape peaks for ...
... peak may be misleading to some . Note that the size of escape - peak pulses corresponds not to the escaping energy , but to the difference between the normal and escaping energies . ) Shown in ( b ) are the normal and escape peaks for ...
Page 231
... peaks are to be recorded and the second when only a few points spanning a specific part of a single peak are to be measured . In general , peaks will be smoothed by modern diffractometer à Imat 1 dvd ( 20 ) 2012 2012 20 20mas 28 ih LA ...
... peaks are to be recorded and the second when only a few points spanning a specific part of a single peak are to be measured . In general , peaks will be smoothed by modern diffractometer à Imat 1 dvd ( 20 ) 2012 2012 20 20mas 28 ih LA ...
Page 232
... peak 20 mid or the midpoint of the points of inflection of the peak 20 infl . An alternative is to calculate the median angle 20 median of the peak , i.e. , the angular position where the area under the peak A , to Al the left of 20 ...
... peak 20 mid or the midpoint of the points of inflection of the peak 20 infl . An alternative is to calculate the median angle 20 median of the peak , i.e. , the angular position where the area under the peak A , to Al the left of 20 ...
Contents
Geometry of Crystals | 31 |
Geometry | 89 |
Intensities Diffraction | 123 |
Copyright | |
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Common terms and phrases
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