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

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Page 270

If the matrix elements for a decay are

straight is a straight line for each such decay [ 29 ] where to get 1 / 35 ( 5 . 4 ) B =

ft [ ( 1 - x ) M ; + « M , nh ? In 2 ( 5 . 5 ) daines = 10 + C ) móc4 ? with gree üzeltid

Fig .

If the matrix elements for a decay are

**known**, then a plot of B vs . x yields astraight is a straight line for each such decay [ 29 ] where to get 1 / 35 ( 5 . 4 ) B =

ft [ ( 1 - x ) M ; + « M , nh ? In 2 ( 5 . 5 ) daines = 10 + C ) móc4 ? with gree üzeltid

Fig .

Page 300

Strange particle , so First we shall survey briefly the major decay modes

for the strange particles , with their decay probabilities as given by experiment .

The main features are summarized in Table I . For the hyperons , pionic decay ...

Strange particle , so First we shall survey briefly the major decay modes

**known**for the strange particles , with their decay probabilities as given by experiment .

The main features are summarized in Table I . For the hyperons , pionic decay ...

Page 327

9 ) W ( K ; → 31 ) ( 1 , + 13 ) ! tudes for \ AT | = { and ; transitions leading to the

final T = 1 state , respectively . Experimentally , the decay probability ( K ; → 3T )

is not yet well

t ...

9 ) W ( K ; → 31 ) ( 1 , + 13 ) ! tudes for \ AT | = { and ; transitions leading to the

final T = 1 state , respectively . Experimentally , the decay probability ( K ; → 3T )

is not yet well

**known**; BARDON et al . [ 8 ] have given the result ( 5 . 10 ) W ( K ) >t ...

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### Contents

GENERALITĄ | 1 |

PARTE PRIMA Problemi teorici | 9 |

PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 251 |

3 other sections not shown

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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 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 respect result scattering shown shows solution space spin spinor symmetry Table theory transformation transition universe vector wave weak zero