Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 77
... tensor product space 1H2 , representing a pair of particles S , and S2 , then a magnitude represented by an operator of the form A1I , ( where A , is maximal in H1 and I , is the unit operator in 2 ) is nonmaximal in the tensor product ...
... tensor product space 1H2 , representing a pair of particles S , and S2 , then a magnitude represented by an operator of the form A1I , ( where A , is maximal in H1 and I , is the unit operator in 2 ) is nonmaximal in the tensor product ...
Page 261
... tensor ( spin 2 ) Jur ( x ) ; 5 ) write the Lagrangian for the free field by invariance arguments ; 6 ) introduce in the Lagrangian interaction with matter by coupling the field to the energy- momentum tensor of matter . Now comes the ...
... tensor ( spin 2 ) Jur ( x ) ; 5 ) write the Lagrangian for the free field by invariance arguments ; 6 ) introduce in the Lagrangian interaction with matter by coupling the field to the energy- momentum tensor of matter . Now comes the ...
Page 408
... tensor and square it , or square the strain tensor and take the trace of it . A linear com- bination of the two quantities with appropriately chosen coefficients gives the most general acceptable expression . By this simple line of ...
... tensor and square it , or square the strain tensor and take the trace of it . A linear com- bination of the two quantities with appropriately chosen coefficients gives the most general acceptable expression . By this simple line 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