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

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Page 34

Then call

of getting the yes outcome of e after interaction with the system prepared

according to n, is the same as after interaction with the system prepared

according to ttt.

Then call

**equivalent**two preparations, say jtj, n„, if, for every eeE, the probabilityof getting the yes outcome of e after interaction with the system prepared

according to n, is the same as after interaction with the system prepared

according to ttt.

Page 152

Whenever n and n' are

obtain equal results from both n and n' . The equivalence relation above defined

is clearly reflexive and symmetric; it is also transitive, because of the transitivity ...

Whenever n and n' are

**equivalent**, one can adjust the units or the scales, so as toobtain equal results from both n and n' . The equivalence relation above defined

is clearly reflexive and symmetric; it is also transitive, because of the transitivity ...

Page 156

When technology advances, and we pass from e to e'<e, we may find that one

and the same quantity splits into two or more quantities, because a number of

procedures, that were e-

has ...

When technology advances, and we pass from e to e'<e, we may find that one

and the same quantity splits into two or more quantities, because a number of

procedures, that were e-

**equivalent**within Zk, are not e'-**equivalent**. This situationhas ...

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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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3-geometry algebra applied assertion atoms axioms Boolean Borel field Borel sets calculus concept conditional probability conditionalization consider corresponding countable course defined definition denote derived deterministic dialog dialog-game disjoint dynamics edited Einstein elements equation equivalent exists experiment finite formal function geometry given Gleason's theorem Hence Hilbert space implies induction initial interaction interpretation irreversible Journ linear magnitude Math mathematical means Neumann non-Boolean notion observable orthogonal orthomodular lattice particle photon Phys physical quantity physical system physical theories physicists positive precision probabilistic probability measure probability space probability theory problem procedure quantum logic quantum mechanics quantum theory quantum-logical question radioactive random variable real numbers relation relative frequency relf represented respect result rule sequence space-time special relativity spin statistical operator subset subspace superspace theorem tion transformation truth universal constants vector velocity von Neumann algebra zero