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

### From inside the book

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Page 56

It is by no means true , that the two

It is by no means true , that the two

**component**theory of Weyl is not compatible with the conservation of parity - this will be shown by proving the ...Page 85

Its

Its

**components**in the general frame of reference ( * ) are denoted by the symbol ... or the x -**component**of the magnetic part of the dual electromagnetic ...Page 171

10-43 cm2 / fission for anti - neutrinos which are described by two

10-43 cm2 / fission for anti - neutrinos which are described by two

**component**wave functions and have only one spin state [ 65 ] ; and ( 181 ) ( 3.05 $ 0.5 ) ...### What people are saying - Write a review

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### Contents

GENERALITÀ | 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 elementary elements 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 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