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

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Page 82

The field leaves foot prints on the

one can almost always read back to get all he needs to know about the

electromagnetic field ( Fig . 6 ) . Even more , one can first check whether the

The field leaves foot prints on the

**curvature**of space so specific that from themone can almost always read back to get all he needs to know about the

electromagnetic field ( Fig . 6 ) . Even more , one can first check whether the

**curvature**of ...Page 84

When this condition is satisfied , then the Einstein

hand side of eq . ( 31 ) reduces to the Ricci

if the

When this condition is satisfied , then the Einstein

**curvature**tensor on the lefthand side of eq . ( 31 ) reduces to the Ricci

**curvature**tensor itself , R , ' . Second ,if the

**curvature**of space is to be attributed to an electromagnetic field , it is also ...Page 100

tities Pmn or Pm " describe the extrinsic

surrounding and still unknown 4 - space . Thus ( 54 ) can be written more

descriptively in this form : ( 55 ) intrinsic

tities Pmn or Pm " describe the extrinsic

**curvature**of this 3 - space in thesurrounding and still unknown 4 - space . Thus ( 54 ) can be written more

descriptively in this form : ( 55 ) intrinsic

**curvature**invariant of o extrinsic**curvature**invariant of o ...### 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