## Proceedings of the International School of Physics "Enrico Fermi.", Volume 70N. Zanichelli, 1978 - Nuclear physics |

### From inside the book

Results 1-3 of 48

Page 191

( 8.15 ) with X , = V.T , one can find the

overshoot as a function of y , for a given H and T : ( 8.16 ) X = ( uHT – My - l4c ) V.

/(V , + uHcb ) . The final

yn = 0 If Hc ...

( 8.15 ) with X , = V.T , one can find the

**position**of the bubble during theovershoot as a function of y , for a given H and T : ( 8.16 ) X = ( uHT – My - l4c ) V.

/(V , + uHcb ) . The final

**position**of the bubble is simply this same equation withyn = 0 If Hc ...

Page 530

This cap is butt - welded again into the crucible in such a

above the melt surface (

by slow cooling — the melt is now saturatedthe crucible is turned into the growth

...

This cap is butt - welded again into the crucible in such a

**position**that the seed isabove the melt surface (

**position**I ) . After spontaneous nucleation has occurredby slow cooling — the melt is now saturatedthe crucible is turned into the growth

...

Page 531

This 50 um thick ( 111 ) wafer has been observed between nearly crossed

polarizers . It clearly shows the growth striations of the cross - sections of the (

211 ) and ( 110 ) growth facets . It shows starting

This 50 um thick ( 111 ) wafer has been observed between nearly crossed

polarizers . It clearly shows the growth striations of the cross - sections of the (

211 ) and ( 110 ) growth facets . It shows starting

**position**I growth**position**II end**position**!### What people are saying - Write a review

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### Contents

Magnetooptical rotation | 2 |

Rareearth iron garnets | 5 |

Bubble translation | 8 |

Copyright | |

35 other sections not shown

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### Common terms and phrases

absorption angle anisotropy Appl applied assumed axis Bloch lines bubble calculated causes centres composition consider constants contribution corresponding coupling crystal cubic curve dependence determined direction discussed distribution domain effects electron energy equation exchange experiment experimental expression Fe2+ Fe3+ ions ferrimagnetic field film function GELLER give given ground increases interaction iron garnets Journ lattice levels light magnetic field magnitude material measurements mode moments motion normal observed obtained occur octahedral orientation parallel parameter photoinduced Phys plane polarization position properties rare-earth ions region relation relaxation represents resonance respectively rotation sample shown in fig shows space group specimens spin wave spontaneous spontaneous magnetization structure sublattice substitution surface symmetry temperature tetrahedral theory tion torque transition uniaxial unit values variation wall yttrium iron garnet

### References to this book

Structural and Magnetic Phase Transitions in Minerals S. Ghose,J.M.D. Coey,E. Salje Snippet view - 1988 |