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 179
... curve . For an incident plane wave and the reflection setting , dynamical theory predicts a flat - topped rocking curve ; the simulation shown in Fig . 5-8 includes the effect of absorption which slightly changes the shape of the top of ...
... curve . For an incident plane wave and the reflection setting , dynamical theory predicts a flat - topped rocking curve ; the simulation shown in Fig . 5-8 includes the effect of absorption which slightly changes the shape of the top of ...
Page 180
... curve for 004 silicon with Mo Ka , radiation and x - ray absorption . If x - ray absorption were absent , the top of the curve would be flat and the curve would be symmetrical . ( Simulation with RADS Software , Bede Scientific ...
... curve for 004 silicon with Mo Ka , radiation and x - ray absorption . If x - ray absorption were absent , the top of the curve would be flat and the curve would be symmetrical . ( Simulation with RADS Software , Bede Scientific ...
Page 567
... curves ( Fig . 19-8 ) . Curve 1 ( dashdotted line ) showed scattered intensity proportional to e for the inner portion of the curve ; pores exist , therefore , that are so large that k Dmin 2 3.5 is always satisfied . Scattering from ...
... curves ( Fig . 19-8 ) . Curve 1 ( dashdotted line ) showed scattered intensity proportional to e for the inner portion of the curve ; pores exist , therefore , that are so large that k Dmin 2 3.5 is always satisfied . Scattering from ...
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