Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 31
... spectra consist of the values 0 and 1 ; they form an ordered struc- ture , technically an orthomodular complete lattice . The operations do not play a very explicit role , but can be associated to the measurement of an ob- servable with ...
... spectra consist of the values 0 and 1 ; they form an ordered struc- ture , technically an orthomodular complete lattice . The operations do not play a very explicit role , but can be associated to the measurement of an ob- servable with ...
Page 74
... spectra cannot be correct in general , for fairly obvious reasons . ( Consider , for example , a « measurement » of the magni- tude represented by the unit operator I on a system in the pure state y . The projection postulate requires ...
... spectra cannot be correct in general , for fairly obvious reasons . ( Consider , for example , a « measurement » of the magni- tude represented by the unit operator I on a system in the pure state y . The projection postulate requires ...
Page 157
... spectra of p . ( x ) and e ( x ) . Since high frequencies are very little , if at all , represented in the Fourier spectrum of e ( x ) , the same can be said for p ( x ) . As a consequence , p ( x ) is a fairly well - behaved function ...
... spectra of p . ( x ) and e ( x ) . Since high frequencies are very little , if at all , represented in the Fourier spectrum of e ( x ) , the same can be said for p ( x ) . As a consequence , p ( x ) is a fairly well - behaved function ...
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