Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
From inside the book
Results 1-3 of 24
Page 56
... orthogonal subset B of P is a basis , i.e. = 0 , every maximally pairwise Σaß ) = 1 for every P. BEB The set ... orthogonal com- plement of any subset A of P as the set of all states orthogonal to every state of A ; we write A ' for this ...
... orthogonal subset B of P is a basis , i.e. = 0 , every maximally pairwise Σaß ) = 1 for every P. BEB The set ... orthogonal com- plement of any subset A of P as the set of all states orthogonal to every state of A ; we write A ' for this ...
Page 58
... orthogonal . Let C be a maximal pairwise orthogonal subset of B ' : then BC is a basis for the whole so that , for every aЄP , Σ <a ẞ> + + Σ < aly > VEC Σ αγ VEC - *** ВЕВ 1. Take now any state a in B ' ; we have Σ < aẞ ) = 0 , hence 1 ...
... orthogonal . Let C be a maximal pairwise orthogonal subset of B ' : then BC is a basis for the whole so that , for every aЄP , Σ <a ẞ> + + Σ < aly > VEC Σ αγ VEC - *** ВЕВ 1. Take now any state a in B ' ; we have Σ < aẞ ) = 0 , hence 1 ...
Page 374
... orthogonal decomposition . P1 , P2 , ... are probability measures on M , then so is ( 5.8 ) ∞ P = Στη Ρη , n = 1 1 , Στ , = 1 . n = 1 I shall call ... orthogonal family , there 374 B. C. VAN FRAASSEN Partition and orthogonal decomposition.
... orthogonal decomposition . P1 , P2 , ... are probability measures on M , then so is ( 5.8 ) ∞ P = Στη Ρη , n = 1 1 , Στ , = 1 . n = 1 I shall call ... orthogonal family , there 374 B. C. VAN FRAASSEN Partition and orthogonal decomposition.
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
29 other sections not shown
Other editions - View all
Common terms and phrases
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