Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 73
... magnitude , might either predict the same , or similar , distribution with nonzero dispersion for the results of an immediate re - measurement of a magnitude A on systems which have all been found to have a particular value a of A , or ...
... magnitude , might either predict the same , or similar , distribution with nonzero dispersion for the results of an immediate re - measurement of a magnitude A on systems which have all been found to have a particular value a of A , or ...
Page 74
... magnitude A ? In the case of a nonmaximal magnitude B , VON NEUMANN argues that an initial statistical operator W is always transformed to a mixture W ' , even if W represents a pure state . How- ever , W ' is not in general uniquely ...
... magnitude A ? In the case of a nonmaximal magnitude B , VON NEUMANN argues that an initial statistical operator W is always transformed to a mixture W ' , even if W represents a pure state . How- ever , W ' is not in general uniquely ...
Page 76
... magnitude A , such that B = f ( A ) , with loss of information . Thus , the measurement procedure for B is only uniquely defined in general by spec- ifying B as a function of some maximal magnitude . The case of a magnitude C with a ...
... magnitude A , such that B = f ( A ) , with loss of information . Thus , the measurement procedure for B is only uniquely defined in general by spec- ifying B as a function of some maximal magnitude . The case of a magnitude C with a ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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3-geometry algebra assertion atoms axioms Boolean Borel field Borel sets calculus classical concept conditional probability conditionalization corresponding countable course defined definition denote derived deterministic dialog dialog-game disjoint dynamics eigenvalue eigenvectors EINSTEIN elementary elements equation equivalent exists finite formal function geometry given Gleason's theorem Hence Hilbert space induction initial interpretation Journ magnitude Math mathematical means NEUMANN observed orthogonal orthomodular lattice particle photon Phys physical quantity physical system physical theories physicists possible postulate precision probabilistic probability measure probability space probability theory problem procedure propositions quantity Q quantum logic quantum mechanics quantum-logical radioactive random variable real numbers relation relative frequency relf represents respect result rule sequence space-time special relativity spin statistical operator structure subset subspace superspace t₁ T₂ theorem tion transformation truth universal constants vector velocity von Neumann algebra