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

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Page 151

When n is applied to a, it yields a

defined later on. ... We shall say that a procedure n is defined with respect to a,

when it can be applied to a, to yield a nonempty set of

When n is applied to a, it yields a

**result**n(a). What exactly is a «**result**» will bedefined later on. ... We shall say that a procedure n is defined with respect to a,

when it can be applied to a, to yield a nonempty set of

**results**nw(a), ...,n<n>(a).Page 159

We will say that n and n' are <e^, e1"} -equivalent with respect to E if and only if, 4

) for every ae E, the application of n and n' to the same parts of a yields the same

number n of

We will say that n and n' are <e^, e1"} -equivalent with respect to E if and only if, 4

) for every ae E, the application of n and n' to the same parts of a yields the same

number n of

**results**^{n>(o) and n'iv(a), ... , n[n>(o), respectively ; B") for every ...Page 165

... the corresponding

denote this

occurring in a, a corresponding deterministic (probabilistic)

D, ...

... the corresponding

**result**for the quantity time (Q„) can be obtained in *; let usdenote this

**result**by <<>„,= tk±e,l2; 2) for ... term d, (fr) (probabilistic term p, (f„))occurring in a, a corresponding deterministic (probabilistic)

**result**for the quantityD, ...

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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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