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

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Page 33

Consequences of Invariance under

Eigenvalues . In contrast to the operator of time reversal the operators of

and charge conjugation are linear and unitary and , therefore , possess ...

Consequences of Invariance under

**Parity**and under Charge Conjugation . 1 . -Eigenvalues . In contrast to the operator of time reversal the operators of

**parity**and charge conjugation are linear and unitary and , therefore , possess ...

Page 34

For the intrinsic

antiparticle ( IV . 8 ) P„ ; - = inn - . Though we did not make that clear in the

notations the ne in general differ from field to field . For the standard form eqs . (

11 . 36 ) , ( II .

For the intrinsic

**parity**we find ( IV . 7 ) PY , + = in . Ve + and for that of theantiparticle ( IV . 8 ) P„ ; - = inn - . Though we did not make that clear in the

notations the ne in general differ from field to field . For the standard form eqs . (

11 . 36 ) , ( II .

Page 35

Only the intrinsic

is defined absolutely ( empirically it is odd ) . The generalized charges one has to

consider in connection with the ambiguities are those which are conserved in ...

Only the intrinsic

**parity**of strictly neutral bosons ( i . e . of the neutral 7° mesong )is defined absolutely ( empirically it is odd ) . The generalized charges one has to

consider in connection with the ambiguities are those which are conserved in ...

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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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### 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 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