## 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 ,

Op ) [ CB ( e , OBv ) + cs ( e , 0Byov ) ] of a linear

constants Cb , Cs ) of products of matrix elements of the independent spinor ...

Thus , the B - decay interaction Lagrangian is usually given in the form L = { { { n ,

Op ) [ CB ( e , OBv ) + cs ( e , 0Byov ) ] of a linear

**combination**( with couplingconstants Cb , Cs ) of products of matrix elements of the independent spinor ...

Page 81

The covariant generalization of the d ' Alembert guy in these equations is

provided by a certain

R . .

The covariant generalization of the d ' Alembert guy in these equations is

provided by a certain

**combination**of first and ... coefficients , or in other words , a**combination**of the Ricci curvature tensor R , and the curvature invariant R = gurR . .

Page 305

n + et tv , for which AQ / As = - 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 ) S + +n + et tv , for which AQ / As = - 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 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