Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 181
... example . Let Q and Q , be two quantities with corresponding operators g ( Q ) and g ( Q ; ) , and let be an ideal physical state such that y , 9 , and y = Y Σε Στ . Χ . where the q , ' s and the x , ' s are respectively eigenvectors of ...
... example . Let Q and Q , be two quantities with corresponding operators g ( Q ) and g ( Q ; ) , and let be an ideal physical state such that y , 9 , and y = Y Σε Στ . Χ . where the q , ' s and the x , ' s are respectively eigenvectors of ...
Page 221
... example is the « reci- procity of relative lengths » : of two identical rods ( i.e. of the same proper- length or ... examples are the « reciprocity of relative time intervals » , the temporal analogue of the preceding , or the ...
... example is the « reci- procity of relative lengths » : of two identical rods ( i.e. of the same proper- length or ... examples are the « reciprocity of relative time intervals » , the temporal analogue of the preceding , or the ...
Page 239
... example of two important constants , c and G. But a first , and simple , example is furnished by the el- ementary charge e . When it first occurred in physics , through the discovery of the electron and the measurement of its charge ...
... example of two important constants , c and G. But a first , and simple , example is furnished by the el- ementary charge e . When it first occurred in physics , through the discovery of the electron and the measurement of its charge ...
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