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

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Page 142

space , but also a great field , as indicated by the lines of force in the enlarged

view of a at the right . Fig . 17 provides a symbolic representation of the typical ...

**Associated**with a typical wormhole such as a is not only a great curvature ofspace , but also a great field , as indicated by the lines of force in the enlarged

view of a at the right . Fig . 17 provides a symbolic representation of the typical ...

Page 158

Therefore an infinite set of rotational degrees of freedom might seem a natural

object to take as progenitor of a spinor field . A simple orthogonal transformation

at one point is

infinitude ...

Therefore an infinite set of rotational degrees of freedom might seem a natural

object to take as progenitor of a spinor field . A simple orthogonal transformation

at one point is

**associated**with one rotation . In general relativity , with itsinfinitude ...

Page 366

In addition , early Cosmotron experiments showed that not enough of the

produced A's were accompanied by observed + + - V's to be in accordance with

the notion of

showed ...

In addition , early Cosmotron experiments showed that not enough of the

produced A's were accompanied by observed + + - V's to be in accordance with

the notion of

**associated**production [ 4 ] . Later , H , bubble chamber data clearlyshowed ...

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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