Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 100
... probability space , without introducing the assump- tion of a randomizing measurement disturbance . Such an assumption is re- quired in order to generate the correct quantum - mechanical properties for conditionalization on the results ...
... probability space , without introducing the assump- tion of a randomizing measurement disturbance . Such an assumption is re- quired in order to generate the correct quantum - mechanical properties for conditionalization on the results ...
Page 371
... space of good family Q. It will be noted from condition ii ) that F is itself a Borel field , for , if A1 , A2 , are ... probability space . For let A1 , A2 , ... be disjoint members of F. Then , by condition ii ) of ( 4.1 ) , there is ...
... space of good family Q. It will be noted from condition ii ) that F is itself a Borel field , for , if A1 , A2 , are ... probability space . For let A1 , A2 , ... be disjoint members of F. Then , by condition ii ) of ( 4.1 ) , there is ...
Page 373
... space in which all relevant sets are full . For let S < K , F , P > be a probability space and S。= ( [ 0 , 1 ] , Bo , μ the unit interval with Lebesgue measure . We form the product space SS , in which the set of points is the ...
... space in which all relevant sets are full . For let S < K , F , P > be a probability space and S。= ( [ 0 , 1 ] , Bo , μ the unit interval with Lebesgue measure . We form the product space SS , in which the set of points is 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