## Treatise on materials science and technology, Volume 4 |

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Page 10

is parallel to [uvw], cones of

near the origin in the N = 0 layer in Fig. 4a. In general there are two differences

between such a

...

is parallel to [uvw], cones of

**diffracted**rays occur, corresponding to the circlesnear the origin in the N = 0 layer in Fig. 4a. In general there are two differences

between such a

**pattern**and the one from a randomly oriented film. The first is that...

Page 13

direction in the real lattice, then an hkl diffraction spot appears in the

7) with N = 0. In the pattern of Fig. 5a, [ww] = [001]. Thus an hkl diffraction spot ...

direction in the real lattice, then an hkl diffraction spot appears in the

**diffraction****pattern**if the following relation is satisfied Equation (9) is the special case of Eq. (7) with N = 0. In the pattern of Fig. 5a, [ww] = [001]. Thus an hkl diffraction spot ...

Page 14

In this way the

determined. 2. Multiple Scattering Under certain conditions extra reflections that

are forbidden by the structure factor appear in the

...

In this way the

**diffraction pattern**for any arbitrary incident beam direction can bedetermined. 2. Multiple Scattering Under certain conditions extra reflections that

are forbidden by the structure factor appear in the

**diffraction pattern**. These extra...

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### Contents

Microstructural Characterization of Thin Films | 2 |

Fundamental Concepts of Diffraction | 4 |

Epitaxial Monocrystalline Films | 10 |

Copyright | |

26 other sections not shown

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### Common terms and phrases

a-sublattice Acta alloys aluminum average beam calculated compaction component compositional dependences compression concentration configurational entropy copper correlation factor crystallites CsCl phases decreases deformation diffraction pattern diffusion coefficient dislocation density disorder parameter effect electron diffraction equations Evans and Flanagan f.c. tetragonal face-centered cubic fiber axis flux forged free energy function Gibbs free energy given increases intermetallic iron powder isostatic jump rate lattice disorder material matrix mechanism nearest neighbor observed obtained occurs oriented partial enthalpy partial entropy Phys plane Poisson ratio polycrystalline probability pure metals random reciprocal lattice relps RHEED shear stress shown in Fig single crystals sintered sintered powder solid solution strengthening solute atoms solute content specimen stacking fault energy stoichiometry stress-strain curve structure sublattice Substituting surface Suzuki TED pattern temperature dependence tetragonal theoretical thermal thermodynamic thermodynamic activities thermodynamic properties thin films tracer jump twin vacancy jumps values variations Vook X-ray yield stress