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

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Page 64

1 )

Y = x1 Q1 to 13 Q3 + yl , ( + xy + y2 = 1 ) , and using ( 73 ) for A ans 8 one finds

that the allowed

1 )

**parameters**in the general and one in the present case . Putting mulie ' s ( 92 )Y = x1 Q1 to 13 Q3 + yl , ( + xy + y2 = 1 ) , and using ( 73 ) for A ans 8 one finds

that the allowed

**parameter**combinations # h as are those represented in the ...Page 157

The coefficients are labelled by two indices , m and m ' , and are functions of the

demands single valued wave functions . The coefficients of transformation must ...

The coefficients are labelled by two indices , m and m ' , and are functions of the

**parameters**of the rotation . In dealing with normal rigid body rotations onedemands single valued wave functions . The coefficients of transformation must ...

Page 326

It says furthermore that the asymmetry

properties of the two modes should be identical . The data on the branching ratio

is not , however , a clear proof that AT1 = } holds , since there is another well -

defined ...

It says furthermore that the asymmetry

**parameters**and other polarizationproperties of the two modes should be identical . The data on the branching ratio

is not , however , a clear proof that AT1 = } holds , since there is another well -

defined ...

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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