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 49
... example , are always į no matter whether the unit cell is cubic , tetragonal , or orthorhombic , and whatever its size . The coordinates of a point position , such as į 1 2 , may also be regarded as an operator which , when “ applied ...
... example , are always į no matter whether the unit cell is cubic , tetragonal , or orthorhombic , and whatever its size . The coordinates of a point position , such as į 1 2 , may also be regarded as an operator which , when “ applied ...
Page 60
... example , is called the A1 structure , a - Fe is A2 , zinc is A3 , diamond is A4 , NaCl is B1 , etc. A full list is given by Pearson ( G.9 , Vol . 1 , p . 85 ) . Some rather complex crystals can be built on a cubic lattice . For example ...
... example , is called the A1 structure , a - Fe is A2 , zinc is A3 , diamond is A4 , NaCl is B1 , etc. A full list is given by Pearson ( G.9 , Vol . 1 , p . 85 ) . Some rather complex crystals can be built on a cubic lattice . For example ...
Page 140
... examples that some of the information given was not used in the calculations . In ( a ) , for example , the cell was said to contain only one atom , but the shape of the cell was not specified ; in ( b ) and ( c ) , the cells were ...
... examples that some of the information given was not used in the calculations . In ( a ) , for example , the cell was said to contain only one atom , but the shape of the cell was not specified ; in ( b ) and ( c ) , the cells were ...
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