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

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Page 85

When a = 0 , the field { e = $ , 0 , 0 ; h = 0 , 0 , 0 } may be said to have a «

electric complexion » . If regarded from a reference system other than the

standard one , the electromagnetic field tensor in this case , Xuve will of course

generally ...

When a = 0 , the field { e = $ , 0 , 0 ; h = 0 , 0 , 0 } may be said to have a «

**purely**electric complexion » . If regarded from a reference system other than the

standard one , the electromagnetic field tensor in this case , Xuve will of course

generally ...

Page 89

The blindness arose only when the two sets of second order equations were

combined into one

truly physical distinction between the complexions in regions A and B even

though ...

The blindness arose only when the two sets of second order equations were

combined into one

**purely**geometrical set of fourth order equations . There is atruly physical distinction between the complexions in regions A and B even

though ...

Page 115

The wormhole allows a

The two far away mouths of a wormhole manifest mass , in the sense that the

metric around each is Schwarzschildean in character , as it is around any « real ...

The wormhole allows a

**purely**geometrical description of a two body problem . –The two far away mouths of a wormhole manifest mass , in the sense that the

metric around each is Schwarzschildean in character , as it is around any « real ...

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### Contents

GENERALITĄ | 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