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

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Page 28

... where « and ß contain the specification of the states besides the angular

momentum . Because of

Ogey · From the way T transforms the operator I . , of angular momentum ( eq . (

11 .

... where « and ß contain the specification of the states besides the angular

momentum . Because of

**rotational**symmetry ( III . 10 ) ( b [ Sla ) = ( B | | 8 , | | 02 ,Ogey · From the way T transforms the operator I . , of angular momentum ( eq . (

11 .

Page 37

The reflected situation is shown in Fig . 5b : the orientation of the initial spins is

the same ; the direction of the momentum of the decay products is reversed .

What matters is , because of

direction of ...

The reflected situation is shown in Fig . 5b : the orientation of the initial spins is

the same ; the direction of the momentum of the decay products is reversed .

What matters is , because of

**rotational**invariance , the angle between thedirection of ...

Page 158

Therefore an infinite set of

object to take as progenitor of a spinor field . A simple orthogonal transformation

at one point is associated with one rotation . In general relativity , with its

infinitude ...

Therefore an infinite set of

**rotational**degrees of freedom might seem a naturalobject to take as progenitor of a spinor field . A simple orthogonal transformation

at one point is associated with one rotation . In general relativity , with its

infinitude ...

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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