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

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Page 116

It follows that the coupling between 8 and a

selects a unique

possibility structure of S 4- M, viz. the subalgebra 3Ss+M generated by the

projection ...

It follows that the coupling between 8 and a

**Boolean**measuring instrument Mselects a unique

**Boolean**subalgebra in the non-**Boolean**propositional orpossibility structure of S 4- M, viz. the subalgebra 3Ss+M generated by the

projection ...

Page 118

The conditional probabilities always refer to the results of a subsequent

measurement B, conditional on a prior measurement A, where the measurements

of A and B involve the selection of two (incompatible)

...

The conditional probabilities always refer to the results of a subsequent

measurement B, conditional on a prior measurement A, where the measurements

of A and B involve the selection of two (incompatible)

**Boolean**subalgebras in the...

Page 301

In classical physics, a property is represented by a subset of the set Q. The set P(

Q) of all subsets of Q is a complete lattice which is a

usual quantum mechanics, a property is represented by an orthogonal projector ...

In classical physics, a property is represented by a subset of the set Q. The set P(

Q) of all subsets of Q is a complete lattice which is a

**Boolean**algebra [1]. In theusual quantum mechanics, a property is represented by an orthogonal projector ...

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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