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

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Page 6

Thus , the B - decay interaction Lagrangian is usually given in the form L ( n , 05p

) [ Cr ( e , Obv ) + 6 ( e , 0By : v ) ] of a linear

Cb , C's ) of products of matrix elements of the independent spinor operator OB ...

Thus , the B - decay interaction Lagrangian is usually given in the form L ( n , 05p

) [ Cr ( e , Obv ) + 6 ( e , 0By : v ) ] of a linear

**combination**( with coupling constantsCb , C's ) of products of matrix elements of the independent spinor operator OB ...

Page 81

... source term in Einstein's equations for the metric which governs the geometry

of space - time . The covariant generalization of the d'Alembert guy in these

equations is provided by a certain

the ...

... source term in Einstein's equations for the metric which governs the geometry

of space - time . The covariant generalization of the d'Alembert guy in these

equations is provided by a certain

**combination**of first and second derivatives ofthe ...

Page 305

et tv , for which AQ / A8 = -1 . There is no experimental data which require the

existence of an interaction leading to processes of this type ; for the particular ...

**Combination**with I would lead , for example , to the decay process ( 1.10 ) + → ntet tv , for which AQ / A8 = -1 . There is no experimental data which require the

existence of an interaction leading to processes of this type ; for the particular ...

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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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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