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

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Page 204

These two independent distributions of the vector J ,

0 , \ JM and < 0,5J M , , give rise to a definite angular distribution of the axis p with

respect to n , which may be written as an expansion in Legendre polynomials ...

These two independent distributions of the vector J ,

**corresponding**to the states (0 , \ JM and < 0,5J M , , give rise to a definite angular distribution of the axis p with

respect to n , which may be written as an expansion in Legendre polynomials ...

Page 223

Quite generally , the state of polarization of a fermion is defined by the relative

amplitudes of the wavefunctions

the spin along an arbitrary spatial axis . By taking as axis of reference the ...

Quite generally , the state of polarization of a fermion is defined by the relative

amplitudes of the wavefunctions

**corresponding**to the two possible orientations ofthe spin along an arbitrary spatial axis . By taking as axis of reference the ...

Page 285

The optimum length of the magnetized absorber can be calculated easily ( 12 ) ,

the

polarization , and saturated iron , is shown in curve a of Fig . 2 as a function of ...

The optimum length of the magnetized absorber can be calculated easily ( 12 ) ,

the

**corresponding**value of d for a completely polarized y - ray with right circularpolarization , and saturated iron , is shown in curve a of Fig . 2 as a function of ...

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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