Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 80
... operators of the form A1I2 [ 11 ] . Similarly , W defines a unique statistical operator W2 of S2 , which specifies the statistics of all magni- tudes represented by operators of the form I1 A2 . Let the matrix of W with respect to the ...
... operators of the form A1I2 [ 11 ] . Similarly , W defines a unique statistical operator W2 of S2 , which specifies the statistics of all magni- tudes represented by operators of the form I1 A2 . Let the matrix of W with respect to the ...
Page 92
... operators » , so that the condition satisfied by the conditionalization map A → A ' cor- responding to the ... operators P. , i = 1 , 2 , ... , then , for each statistical operator W , a generalized conditional expectation is defined by ...
... operators » , so that the condition satisfied by the conditionalization map A → A ' cor- responding to the ... operators P. , i = 1 , 2 , ... , then , for each statistical operator W , a generalized conditional expectation is defined by ...
Page 93
... operator can be represented as a weighted sum of orthogonal projection operators , every statistical operator can be generated by conditionalizing a 1 - dimensional projection operator representing an atomic property or event with ...
... operator can be represented as a weighted sum of orthogonal projection operators , every statistical operator can be generated by conditionalizing a 1 - dimensional projection operator representing an atomic property or event with ...
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