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

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Page 83

Poynting flux will be

units cm - ? ) will therefore be parallel . Let the axis to which they are parallel be

called the x ' axis . Then in this frame of reference all components of the stress ...

Poynting flux will be

**zero**( * ) . The electric and magnetic fields ( e ' and h ' inunits cm - ? ) will therefore be parallel . Let the axis to which they are parallel be

called the x ' axis . Then in this frame of reference all components of the stress ...

Page 184

ration between positive and negative energy states goes to

the transition depend upon the equation of state assumed , but the existence of

the effects does not ( * ) . Fig . 22 describes a configuration short of the crimca 1V

...

ration between positive and negative energy states goes to

**zero**. The details ofthe transition depend upon the equation of state assumed , but the existence of

the effects does not ( * ) . Fig . 22 describes a configuration short of the crimca 1V

...

Page 354

Let us consider the total « charge » Q . Then Q applied to a nucleon at rest has to

give another state with total momentum

such states exist unless one neglects the hyperon nucleon mass differences .

Let us consider the total « charge » Q . Then Q applied to a nucleon at rest has to

give another state with total momentum

**zero**but with non -**zero**strangeness . Nosuch states exist unless one neglects the hyperon nucleon mass differences .

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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 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 nucleons 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 requires respect result scattering shown shows solution space spin symmetry Table theory transformation transitions universe vector wave weak zero