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

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Page 29

Decay problems .

only be studied in decay processes . S matrix theory is not directly applicable on

decay processes since only states of stable particles can occur as initial or final ...

Decay problems .

**Weak**interactions can , because of their**weakness**, practicallyonly be studied in decay processes . S matrix theory is not directly applicable on

decay processes since only states of stable particles can occur as initial or final ...

Page 332

B In summary , we repeat that the success of the ( 1 - 1 )

current hypothesis for B - decay , p - decay and i - - capture has led to the

suggestion that it should be extended to strange particle decay processes . We

have seen that ...

B In summary , we repeat that the success of the ( 1 - 1 )

**weak**- interactioncurrent hypothesis for B - decay , p - decay and i - - capture has led to the

suggestion that it should be extended to strange particle decay processes . We

have seen that ...

Page 339

If S were coupled , then by coupling it with Si + 1 ) one would have

interactions with AS = £2 , which seem to be excluded experimentally Now what

about neutral current ? One can define a neutral lepton current pro countaining (

vv ) , ( e ...

If S were coupled , then by coupling it with Si + 1 ) one would have

**weak**interactions with AS = £2 , which seem to be excluded experimentally Now what

about neutral current ? One can define a neutral lepton current pro countaining (

vv ) , ( e ...

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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 element elementary 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 question 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