## Treatise on Materials Science and Technology, Volume 4 |

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Page 5

Similarly , the reciprocal

Similarly , the reciprocal

**lattice**points ( relps ) are given by r * ( hkl ) ha * + kb * + lc * , where the a * , b * , and c * vectors constitute the ...Page 7

Thus a HEED pattern closely represents a plane of the reciprocal

Thus a HEED pattern closely represents a plane of the reciprocal

**lattice**in the region near the transmitted beam . The value of JE , n , 0 ) corresponding ...Page 67

The jump rate depends upon the sequence of atomic events which ultimately leads to atomic displacement from one to an adjacent

The jump rate depends upon the sequence of atomic events which ultimately leads to atomic displacement from one to an adjacent

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### Contents

RICHARD W VOOK | 2 |

Epitaxial Monocrystalline Films | 10 |

Polycrystalline Films | 37 |

Copyright | |

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activity addition alloys applied approximation average beam becomes calculated compaction component composition compression concentration considered constant copper correlation corresponding crystal cubic curve decreases defined deformation density dependence determined diffraction diffusion direction discussed dislocation disorder distribution effect electron elements energy enthalpy entropy equations example experimental expression factor fault field Figure forged function given gives increases influence interaction jump lattice material measurements mechanism metal method neighbor observed obtained occurs oriented parameter partial pattern phases Phys plane polycrystalline position possible powder present probability production properties random ratio reflections region relative respectively shown in Fig shows single crystals sintered solid solution solute atoms solvent specimen strain strengthening stress structure Substituting surface Table temperature theoretical theory thermodynamic thin films tracer twin vacancy values variations volume yield