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

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Page 30

Besides the fact that the point where the definition of system ends and the

definition of state begins is, to a good extent, a matter of taste, some idealization

emerges when the

used to ...

Besides the fact that the point where the definition of system ends and the

definition of state begins is, to a good extent, a matter of taste, some idealization

emerges when the

**notion**of state is thought of in terms of the procedure to beused to ...

Page 62

2 P| ^,(a), we conclude that the orthoclosed subsets are precisely the subsets

which are closed with respect to Varadarajan's

in sect. 3, J5f,(a) stands for {A e &(&>):*(A) = 1}). Deltyannis [31] has shown how

to ...

2 P| ^,(a), we conclude that the orthoclosed subsets are precisely the subsets

which are closed with respect to Varadarajan's

**notion**of state superposition (asin sect. 3, J5f,(a) stands for {A e &(&>):*(A) = 1}). Deltyannis [31] has shown how

to ...

Page 120

In the quantum-mechanical terminology: the

a to b, to be denoted by P(a, b), must bo introduced. P(a, b) is the probability of b,

if a is known to be true. P(o, b) can be used to define a< b and — a: P(o, b) = 1 ...

In the quantum-mechanical terminology: the

**notion**of 'transition probability' froma to b, to be denoted by P(a, b), must bo introduced. P(a, b) is the probability of b,

if a is known to be true. P(o, b) can be used to define a< b and — a: P(o, b) = 1 ...

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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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