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

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Page 30

If the strong interactions are irrelevant for the process under consideration phasiz

orde ( III . 17 ) < a | 8 , 16 ) = ( a 16 ) er der one

( * ) I low 0 ( I11 . 18 ) ( a [ MK , = { Ta | M | Tk * . white , immed 18 dec of oth ...

If the strong interactions are irrelevant for the process under consideration phasiz

orde ( III . 17 ) < a | 8 , 16 ) = ( a 16 ) er der one

**finds**the particularly simple result( * ) I low 0 ( I11 . 18 ) ( a [ MK , = { Ta | M | Tk * . white , immed 18 dec of oth ...

Page 337

The B - decay hamiltonian must therefore have the form ( 6 ) where the coupling

constant has been called V & G to respect old traditions . This is the A – ”

coupling . If n and p are antifermions one

, which ...

The B - decay hamiltonian must therefore have the form ( 6 ) where the coupling

constant has been called V & G to respect old traditions . This is the A – ”

coupling . If n and p are antifermions one

**finds**instead V & G ( 9 . 7 , āy ) ( , 797 . ), which ...

Page 358

Integrating over dx one

in the 10 - ja ) ( 019 ( x ) = ) = 0 , ( 3 . 18 ) which shows that this contribution is

zero . Now the last two terms . They contain 8 ( t ) and 8 ( t ) . By partial integration

...

Integrating over dx one

**finds**that Z must be a one pion state . But for such a statein the 10 - ja ) ( 019 ( x ) = ) = 0 , ( 3 . 18 ) which shows that this contribution is

zero . Now the last two terms . They contain 8 ( t ) and 8 ( t ) . By partial integration

...

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### Contents

GENERALITÀ | 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