## Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |

### From inside the book

Results 1-3 of 9

Page 109

A similar f factor determines the

non - negligible value of f , the nucleus or atom should be tightly bound in a solid

and the y - ray energy should be low ( in practice Ž 100 keV ) . In addition ...

A similar f factor determines the

**probability**for resonant absorption . Thus for anon - negligible value of f , the nucleus or atom should be tightly bound in a solid

and the y - ray energy should be low ( in practice Ž 100 keV ) . In addition ...

Page 121

Finally for a disordered magnetic alloy where there may exist a continuous

distribution of hyperfine fields represented by a

function may be approximated by a set of trigonometrical functions the

coefficients of ...

Finally for a disordered magnetic alloy where there may exist a continuous

distribution of hyperfine fields represented by a

**probability**function P ( H ) , thisfunction may be approximated by a set of trigonometrical functions the

coefficients of ...

Page 237

If m , > m 2 , however , the signs of V 1 , and v1 , are the same and the sputtering

gas atom will not be reflected by the first collision , which greatly reduces the

If m , > m 2 , however , the signs of V 1 , and v1 , are the same and the sputtering

gas atom will not be reflected by the first collision , which greatly reduces the

**probability**it will ever achieve a high energy trajectory away from the target and ...### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

R JAMES | 2 |

Principles of XRay Stress Measurement | 4 |

Control of Accuracy and Precision | 25 |

Copyright | |

15 other sections not shown

### Other editions - View all

### Common terms and phrases

absorption additional allows alloy angle Appl applications atoms bandgap beam broadening cause coefficients components composition composition profile concentration constant containing cooling crystal curve defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distance distribution effect electron elements employed energy error et al example excitation experimental factor field function give given grain heat important included increasing intensity intensity bands iron laser lattice layer less magnetic material measurements Metals method Mössbauer observed obtained occur optical parameter peak phase Phys plane position possible powder problem produce range rays recent region relative residual stress sample semiconductors shift shown single Society solid spacing specimen spectra spectrum sputtering steel structure studies substrate surface target technique temperature term thickness values variation volume x-ray