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

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Page 83

Then in this frame of

hand side of (31)) vanish except these (Table II): Table II. - The non-zero

components of the Maxwell stress-energy tensor for a normal electromagnetic

field as ...

Then in this frame of

**reference**all components of the stress-energy tensor (righthand side of (31)) vanish except these (Table II): Table II. - The non-zero

components of the Maxwell stress-energy tensor for a normal electromagnetic

field as ...

Page 84

Then there exists at each point P in the space-time region in question a suitable

Lorentz

are diagonal at this point in this

...

Then there exists at each point P in the space-time region in question a suitable

Lorentz

**reference**system LF, such that the Eicci and Einstein curvature tensorsare diagonal at this point in this

**reference**system, with diagonal elements (— £a,...

Page 85

write in this particular frame of

where the angle <x defines the complexion. A few comments may be made about

the complexion of an electromagnetic field. When a = 0, the field {e = f , 0, 0 ; h ...

write in this particular frame of

**reference**(39) e = (f, 0, 0) cos a , h = (f, 0, 0) sin a ,where the angle <x defines the complexion. A few comments may be made about

the complexion of an electromagnetic field. When a = 0, the field {e = f , 0, 0 ; h ...

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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