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

### From inside the book

Results 1-3 of 67

Page 23

A second question ig whether advantage can be taken of these ambiguities to

factors. For this purpose we form the squares of the symmetry operations (11.34)

P'3 ...

A second question ig whether advantage can be taken of these ambiguities to

**obtain**certain standard forms of the operations with particularly simple phasefactors. For this purpose we form the squares of the symmetry operations (11.34)

P'3 ...

Page 46

It can now be easily verified on the basis of the commutation relations (19) that it

is possible to

F=-^{l + iy't). The representation which satisfies the reality condition (22) has ...

It can now be easily verified on the basis of the commutation relations (19) that it

is possible to

**obtain**a set of y, starting from Dirac's choice and putting in (20) (23)F=-^{l + iy't). The representation which satisfies the reality condition (22) has ...

Page 357

... identify the lepton Heisenberg operator in the neutrino current with its

corresponding « out » operator to

that of evaluating the vertex (3.8) <*| «£(<)) |Z> of the strangeness non-

conserving current ...

... identify the lepton Heisenberg operator in the neutrino current with its

corresponding « out » operator to

**obtain**(3.7). The whole problem is reduced tothat of evaluating the vertex (3.8) <*| «£(<)) |Z> of the strangeness non-

conserving current ...

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### Contents

GENERALITĄ | 1 |

PARTE PRIMA Problemi teorici | 9 |

PARTE SECONDA Correlazioni angolari polarizzazioni e decadimenti beta | 251 |

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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