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

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Page 45

The use of a symbol different from D stresses the fact that the D-

defined on the flats, hence on the lattice L(&), while the r-

every subset of states, hence on the geometry G(0"). The number r(&) = = D(&) is

the ...

The use of a symbol different from D stresses the fact that the D-

**function**isdefined on the flats, hence on the lattice L(&), while the r-

**function**is defined onevery subset of states, hence on the geometry G(0"). The number r(&) = = D(&) is

the ...

Page 86

The statistical operator construction allows the replacement of the measure

subsets of X, by a corresponding random variable W, a point

domain is A'.

The statistical operator construction allows the replacement of the measure

**function**fi, which is a set**function**whose domain is the field of measurablesubsets of X, by a corresponding random variable W, a point

**function**whosedomain is A'.

Page 442

we have for the ground state probability amplitude

f1, f„ ...) = JV exp[- g- £- ...] . More familiar in the case of the electromagnetic field

than this description in terms of oscillator amplitudes is the so-called occupation ...

we have for the ground state probability amplitude

**function**the expression (37) y(f1, f„ ...) = JV exp[- g- £- ...] . More familiar in the case of the electromagnetic field

than this description in terms of oscillator amplitudes is the so-called occupation ...

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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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