## Proceedings of the International School of Physics "Enrico Fermi.", Volume 11N. Zanichelli, 1960 - Nuclear physics |

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Page 236

In J → J transitions , on the other hand , both types of interaction will in general

of « pure Fermi » , « pure Gamow Teller » and « mixed >>

In J → J transitions , on the other hand , both types of interaction will in general

**contribute**both « pure >> ( r == qo ... We may accordingly speak in a general wayof « pure Fermi » , « pure Gamow Teller » and « mixed >>

**contributions**to the ...Page 307

( ū ( 1 – 7 : ) pt ) , where the constant A. , represents the

intermediate baryon - pair states which lead to the ti - l ... However the set of

intermediate baryon - pair states which

that which ...

( ū ( 1 – 7 : ) pt ) , where the constant A. , represents the

**contribution**of theintermediate baryon - pair states which lead to the ti - l ... However the set of

intermediate baryon - pair states which

**contribute**to K , 2 decay is different fromthat which ...

Page 357

The first term of ( 3.11 ) does not

terms can be shown to give

the subtraction constant of the dispersion relations ; the second term has the right

...

The first term of ( 3.11 ) does not

**contribute**to the matrix element ; the last twoterms can be shown to give

**contributions**which can be thought of as included inthe subtraction constant of the dispersion relations ; the second term has the right

...

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### Contents

GENERALITĄ | 1 |

PARTE PRIMA Problemi teorici | 9 |

PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 197 |

4 other sections not shown

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### Common terms and phrases

allowed angle angular assumed calculated charge classical combination completely component connection conservation consider constant contribute correlation corresponding coupling curvature decay defined density dependence derived described determination direction discussed effects electric electromagnetic field electron elementary elements emission energy equations example existence experiment experimental expression factor Fermi field final finds formula function geometrodynamics geometry give given gravitational histories initial interaction invariance known leads limit magnetic mass matrix means measured metric modes momentum neutrino neutron nuclei nucleons observed obtained operators pairs parity particle phase Phys physics polarization possible present principle problem properties purely quantity quantum quantum mechanics radiation ratio reason reference relation relativity requires respect result scattering shown shows solution space spin symmetry Table theory transformation transitions universe vector wave weak zero