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

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Page 88

How then can these equations be made to appear natural ? Or if they cannot ,

what conclusion can be drawn from this circumstance ! SHARP [ 12 ] has

suggested the possibility that the structure equations can be

variational ...

How then can these equations be made to appear natural ? Or if they cannot ,

what conclusion can be drawn from this circumstance ! SHARP [ 12 ] has

suggested the possibility that the structure equations can be

**derived**from thevariational ...

Page 91

The equations of motion cannot be

equations are linear . The equations of electrodynamics , for example , allow the

field to be calculated from the motion of the charge just as well for an impossible

...

The equations of motion cannot be

**derived**from the field equations if the fieldequations are linear . The equations of electrodynamics , for example , allow the

field to be calculated from the motion of the charge just as well for an impossible

...

Page 249

( 133 ) , ( 134 ) the expressions

the correlation function pertaining to a J - > ) transition 1J + 1 ) J 1 / ( 2 . 5 + 1 ) –

ko lah ( 145 ) W ' ( Onrg ( rp ) = laot 2VJ ( J + 1 ) ll ( 2k - 1 ) ( 2k + 1 ) 1 “ · [ P { ( cos

0 ...

( 133 ) , ( 134 ) the expressions

**derived**for the l ' s , G ' s and D ' s , one finds forthe correlation function pertaining to a J - > ) transition 1J + 1 ) J 1 / ( 2 . 5 + 1 ) –

ko lah ( 145 ) W ' ( Onrg ( rp ) = laot 2VJ ( J + 1 ) ll ( 2k - 1 ) ( 2k + 1 ) 1 “ · [ P { ( cos

0 ...

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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