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

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Page 10

In the following we shall assume that there exists an

the substitution eq . ... Anti - linear

A0 , A2Y = 2 * AY , where l and 0 are state vectors and ą is a c - number .

In the following we shall assume that there exists an

**operator**which generatesthe substitution eq . ... Anti - linear

**operators**( * ) A satisfy ( I . 3 ) A ( Y + 0 ) = AY +A0 , A2Y = 2 * AY , where l and 0 are state vectors and ą is a c - number .

Page 19

2 ) They are local in the sense that they transform positive and negative

frequency parts of the field

« as a whole » ) ( * ) . The reason for the second postulate appears to be that only

for ...

2 ) They are local in the sense that they transform positive and negative

frequency parts of the field

**operators**in the same way ( the fields are transformed« as a whole » ) ( * ) . The reason for the second postulate appears to be that only

for ...

Page 22

It shall be called Fermi

shown to be unitary and because of ( II . ... With the actual relation between spins

and charges occuring in nature F can be expressed by the

...

It shall be called Fermi

**operator**and is defined by ( II . ... The**operator**F can beshown to be unitary and because of ( II . ... With the actual relation between spins

and charges occuring in nature F can be expressed by the

**operators**of baryonic...

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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