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

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Page 236

In J J transitions , on the other hand , both types of interaction will in general

« pure Fermi » , « pure Gamow Teller » ) and « mixed »

double ...

In J J transitions , on the other hand , both types of interaction will in general

**contribute**both « pure » » ( r = . ... We may accordingly speak in a general way of« pure Fermi » , « pure Gamow Teller » ) and « mixed »

**contributions**to thedouble ...

Page 307

However the set of intermediate baryon - pair states which

is different from that which

- meson parity ( relative to that for the A hyperon ) may not be the same as the ...

However the set of intermediate baryon - pair states which

**contribute**to Kit decayis different from that which

**contributes**to Torta decay ; it is also possible that the K- meson parity ( relative to that for the A hyperon ) may not be the same as the ...

Page 357

11 ) does not

give

of the dispersion relations ; the second term has the right form of an advanced ...

11 ) does not

**contribute**to the matrix element ; the last two terms can be shown togive

**contributions**which can be thought of as included in the subtraction constantof the dispersion relations ; the second term has the right form of an advanced ...

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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