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

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Page 82

In other words, if the measuring instrument is represented initially by the

p, then the measurement process is an ... is that there exist measuring

instruments in this sense: Given a complete orthonormal set of

the Hilbert ...

In other words, if the measuring instrument is represented initially by the

**vector**<p, then the measurement process is an ... is that there exist measuring

instruments in this sense: Given a complete orthonormal set of

**vectors**{a,} in Jf, (the Hilbert ...

Page 268

If a quantum- mechanical system is described by a state

equation pA(p = <p (eigenvalue 1) means that <p e A, and the equation PA<p = 0

(eigenvalue 0) that <pB->A, which means that the

the ...

If a quantum- mechanical system is described by a state

**vector**<p e Jt?, theequation pA(p = <p (eigenvalue 1) means that <p e A, and the equation PA<p = 0

(eigenvalue 0) that <pB->A, which means that the

**vector**<p has no component inthe ...

Page 428

He derived electrodynamics and general relativity, or vacuum geometrodynamies

— and the combined theory of the two fields together — by postulating the

simplest action principle that depends on a 4-dimensional

on a ...

He derived electrodynamics and general relativity, or vacuum geometrodynamies

— and the combined theory of the two fields together — by postulating the

simplest action principle that depends on a 4-dimensional

**vector**field (13) K oron a ...

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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