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

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Page 57

Here A = ( ) necessarily , and S

simply : 6 i las fr ( 60 ) y ' = = exp [ iy50 ] * This i - What are the properties of a free

Majorana field which is invariant under ( 60 ) ? If the theory is invariant , its

equations ...

Here A = ( ) necessarily , and S

**becomes**a number a . ( 59 ) then**becomes**simply : 6 i las fr ( 60 ) y ' = = exp [ iy50 ] * This i - What are the properties of a free

Majorana field which is invariant under ( 60 ) ? If the theory is invariant , its

equations ...

Page 119

The regular Kruskal - Schwarzschild metric eventually

finite proper time the curvature invariants - quantities independent of the co -

ordinate system in use —

68 ) .

The regular Kruskal - Schwarzschild metric eventually

**becomes**singular . ... of afinite proper time the curvature invariants - quantities independent of the co -

ordinate system in use —

**become**infinite , corresponding to the point p = 0 in (68 ) .

Page 124

As a consequence the sphere will slowly change shape and

In this case some circumstantial evidence can be cited to suggest that the

intrinsic geometry always

As a consequence the sphere will slowly change shape and

**become**singular . ...In this case some circumstantial evidence can be cited to suggest that the

intrinsic geometry always

**becomes**singular within a finite proper time . 10 * 7 .### 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 | 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