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

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Page 276

This can neither be represented as Fierz interference nor as outer screening

correlations to the spectral shape would be too small to explain the observed

This can neither be represented as Fierz interference nor as outer screening

**effects**since such**effects**would show ... Also**effects**from finite wavelengthcorrelations to the spectral shape would be too small to explain the observed

**effect**.Page 369

Future attempts to observe Ko - Ko interference

additional

in the particle mixture . CASE [ 13 ] and later Goop [ 14 ] have studied these

Future attempts to observe Ko - Ko interference

**effects**must also contend withadditional

**effects**which alter the magnitudes and the phases of the componentsin the particle mixture . CASE [ 13 ] and later Goop [ 14 ] have studied these

**effects**.Page 378

Of course the tripletsinglet transition probability has at least to be comparable to

the capture and decay probabilities for the observation of this

correlation of the recoil neutron . The recoil correlation , for unpolarized protons ...

Of course the tripletsinglet transition probability has at least to be comparable to

the capture and decay probabilities for the observation of this

**effect**. 3. - Angularcorrelation of the recoil neutron . The recoil correlation , for unpolarized protons ...

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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