## Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |

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Page 98

where a, represents the ,S'-property «

represents the ,S"-property «

mechanics, the joint probability pv(a1 & c[) is equal to the sequential probability

— c[), the ...

where a, represents the ,S'-property «

**spin**up in the a-direction » and c[represents the ,S"-property «

**spin**up in the c-direction ». According to quantummechanics, the joint probability pv(a1 & c[) is equal to the sequential probability

— c[), the ...

Page 105

The simplest case is a pair of

= — ja,®*; — y2<*t® *', , where a,, at are eigenvectors of a

The simplest case is a pair of

**spin**- J particles, 8 and 8', in the singlet**spin**state: „= — ja,®*; — y2<*t® *', , where a,, at are eigenvectors of a

**spin**magnitude A of 8 (**spin**in the direction a), and ocj, x'„ are eigenvectors of the corresponding**spin**...Page 185

Let us consider the following atomic sentences of L*\ d,= r, (the value for the ^-

component of

= r„ (the value for the z-component of

Let us consider the following atomic sentences of L*\ d,= r, (the value for the ^-

component of

**spin**is + J) , d, = r, (the value for the z-component of**spin**is + J) , dj= r„ (the value for the z-component of

**spin**is — I) . We will have (84) not '=dj=r1 ...### What people are saying - Write a review

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### Contents

E Amaldi Radioactivity a pragmatic pillar of probabilistic | 1 |

Statistical fluctuations | 10 |

Final remarks | 21 |

Copyright | |

24 other sections not shown

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