Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 34
... interaction with the system prepared according to л , is the same as after inter- action with the system prepared according to 72. Finally , call states of the system the equivalence classes of II ; let be the set of all states , and ...
... interaction with the system prepared according to л , is the same as after inter- action with the system prepared according to 72. Finally , call states of the system the equivalence classes of II ; let be the set of all states , and ...
Page 109
... interaction yields the transition i Yo = - Y Qo U ( t - to , y ( t ) = Σ ( αι , ψ ) α , Qi . Now , the instrument M is a macrosystem . If M has functioned properly , we expect that after the interaction M has registered a particular ...
... interaction yields the transition i Yo = - Y Qo U ( t - to , y ( t ) = Σ ( αι , ψ ) α , Qi . Now , the instrument M is a macrosystem . If M has functioned properly , we expect that after the interaction M has registered a particular ...
Page 116
... interaction between S and a classical , i.e. Boolean , measuring instrument M. Since W ( the statistical operator of SM after the measurement interaction ) defines a classical probability meas- ure on the Boolean subalgebra Bs + M , the ...
... interaction between S and a classical , i.e. Boolean , measuring instrument M. Since W ( the statistical operator of SM after the measurement interaction ) defines a classical probability meas- ure on the Boolean subalgebra Bs + M , the ...
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