Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 152
... defined by CC , C2 with respect to ΣE , UE . 2 = We are now in a position to formulate a generalized operational definition of a physical quantity . A physical quantity Q is defined by the union CU { C } over a set { C } of equivalence ...
... defined by CC , C2 with respect to ΣE , UE . 2 = We are now in a position to formulate a generalized operational definition of a physical quantity . A physical quantity Q is defined by the union CU { C } over a set { C } of equivalence ...
Page 301
... defined on the Hilbert space H. The set P ( H ) of all orthogonal pro- jectors defined on H is a complete lattice too . In general , in quantum physics , a property is represented by a family of orthogonal projectors { Pa } , each Px ...
... defined on the Hilbert space H. The set P ( H ) of all orthogonal pro- jectors defined on H is a complete lattice too . In general , in quantum physics , a property is represented by a family of orthogonal projectors { Pa } , each Px ...
Page 304
... defined a.e. as Xs , ( x ) • = { " 1 if xɛ Дt , if x ¢ 4+ . Secondly , for the momentum p , the complete Boolean lattice is defined as the lattice of the Borel sets in R3 modulo the Borel sets of Lebesgue measure zero and the momentum ...
... defined a.e. as Xs , ( x ) • = { " 1 if xɛ Дt , if x ¢ 4+ . Secondly , for the momentum p , the complete Boolean lattice is defined as the lattice of the Borel sets in R3 modulo the Borel sets of Lebesgue measure zero and the momentum ...
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