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

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Page 441

There we write the wave function of a typical state, for example the

in the form (36) ip(x) = N exp [- mojx*l2h] , where N is a normalization factor. We

proceed similarly with a collection of harmonic oscillators; and with suitably ...

There we write the wave function of a typical state, for example the

**ground state**,in the form (36) ip(x) = N exp [- mojx*l2h] , where N is a normalization factor. We

proceed similarly with a collection of harmonic oscillators; and with suitably ...

Page 442

we have for the

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 ...

Page 487

[173] K. Kuchar:

. Math. Phys., 11, 3322-3334 (1970). [174] C. M. Patton and J. A. Wheeler: ref. [37

], pp. 577 ff. [175] E. Mach: Beiträge zur Analyse der Empfindungen (Jena, 1886 ...

[173] K. Kuchar:

**Ground state**functional of the linearized gravitational field, Journ. Math. Phys., 11, 3322-3334 (1970). [174] C. M. Patton and J. A. Wheeler: ref. [37

], pp. 577 ff. [175] E. Mach: Beiträge zur Analyse der Empfindungen (Jena, 1886 ...

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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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