Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 73
... measurement of a magnitude A on systems which have all been found to have a particular value a of A , or predict the value a of A with no dispersion . The first possibility corresponds to the Bohr- Kramers - Slater theory , which is ...
... measurement of a magnitude A on systems which have all been found to have a particular value a of A , or predict the value a of A with no dispersion . The first possibility corresponds to the Bohr- Kramers - Slater theory , which is ...
Page 74
... measurement which localizes the value c of C to the set S , the state vector of the system can be anywhere in the subspace ( S ) , the range of the projection operator P ( S ) in the spectral measure of C ( where C = frdP ( r ) ) . This ...
... measurement which localizes the value c of C to the set S , the state vector of the system can be anywhere in the subspace ( S ) , the range of the projection operator P ( S ) in the spectral measure of C ( where C = frdP ( r ) ) . This ...
Page 78
... measurement result , can be taken as a general rule , applying to all cases . An A - measurement with loss of information is different from an auton- omous B - measurement , even though the subspace corresponding to the set of ...
... measurement result , can be taken as a general rule , applying to all cases . An A - measurement with loss of information is different from an auton- omous B - measurement , even though the subspace corresponding to the set of ...
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