Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 55
... pair ( L , S ) endowed with the following structure : i ) ii ) is an orthomodular atomic lattice with the covering property ; is a σ - convex set of probability measures on L , and is connected with the order relation of L through ab if ...
... pair ( L , S ) endowed with the following structure : i ) ii ) is an orthomodular atomic lattice with the covering property ; is a σ - convex set of probability measures on L , and is connected with the order relation of L through ab if ...
Page 105
... pair of correlated systems . The simplest case is a pair of spin - particles , S and S ' , in the singlet spin state : 1 1 Y - V2 αι χ a's - ai 1 where α1 , 2 are eigenvectors of a spin magnitude A of S ( spin in the direction a ) , and ...
... pair of correlated systems . The simplest case is a pair of spin - particles , S and S ' , in the singlet spin state : 1 1 Y - V2 αι χ a's - ai 1 where α1 , 2 are eigenvectors of a spin magnitude A of S ( spin in the direction a ) , and ...
Page 126
... pair ( L , S ) which we talked of at the beginning . For convenience we recall here some definitions from orthomodular - lattice theory and measure theory on orthomodular lattices . For details we refer to the existing literature ...
... pair ( L , S ) which we talked of at the beginning . For convenience we recall here some definitions from orthomodular - lattice theory and measure theory on orthomodular lattices . For details we refer to the existing literature ...
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