## Proceedings of the International School of Physics "Enrico Fermi.", Volume 37N. Zanichelli, 1967 - Nuclear physics |

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Results 1-3 of 18

Page 80

for the reflection

Replacing the medium by a continuum , then , the outgoing wave outside R , is

given by ( 4 . 4 ) fe ( r ) lr > R , = h , ( kr ) where for complex k we define h , by its ...

for the reflection

**coefficient**for a fixed E , not the propagation in time for a fixed k .Replacing the medium by a continuum , then , the outgoing wave outside R , is

given by ( 4 . 4 ) fe ( r ) lr > R , = h , ( kr ) where for complex k we define h , by its ...

Page 213

El It is noted here that these equations have the same form as ( 2 . 15 ) . If we

replace U as the

appearance ...

El It is noted here that these equations have the same form as ( 2 . 15 ) . If we

replace U as the

**coefficient**of n , in ( 2 . 15 ) by ( 9U — 4J ) and U as the**coefficient**of m , by ( U + 4J ) we get ( 2 . 22 ) . Therefore , the condition for theappearance ...

Page 405

An explicit expression for the

IZUYAMA , Kim and KUBO [ 14 ] who obtained D = D , ( 1 + E , T } + E , T2 + 0 ( T

? ) ) . These authors assumed a single conduction band and a simplified electron

...

An explicit expression for the

**coefficient**was derived within that framework byIZUYAMA , Kim and KUBO [ 14 ] who obtained D = D , ( 1 + E , T } + E , T2 + 0 ( T

? ) ) . These authors assumed a single conduction band and a simplified electron

...

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### Contents

LOMER Band theory and magnetism | 1 |

PHILLIPS Band theory of transition metals | 22 |

JACCARINO Studies of the hyperfine interaction in transi | 39 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

alloys appearance approximation assume average band becomes bound boundary calculation charge complex computed condition conduction consider contribution correct correlation corresponding coupling curve defined density depends determined direction discussed effect electrons energy equation exchange existence expected expression fact factor Fermi Fermi level Fermi surface ferromagnetic field function given gives Hamiltonian host metal impurity atom increases integral interaction interesting lattice limit localized magnetic matrix elements means method moments normal Note observed obtained occur operator orbital perturbation phase Phys physical plane polarization poles positive possible potential present problem properties range relation replaced represent resonance scattering screening Sect shift shown similar simple single solution spin strong structure temperature theory tion transition metals usual wave wave functions write zero