Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 90
... k , ii ) Exp ( AI ) = Exp ( A'I ) , for all Ye F ' or , alternatively , μ ii ' ) Exp1 ( AZ ) = Exp , ( A'Z ) for every bounded random variable Z that is F - measurable . Such a random variable always exists , but is not unique . If A ...
... k , ii ) Exp ( AI ) = Exp ( A'I ) , for all Ye F ' or , alternatively , μ ii ' ) Exp1 ( AZ ) = Exp , ( A'Z ) for every bounded random variable Z that is F - measurable . Such a random variable always exists , but is not unique . If A ...
Page 333
... exp [ — H / kT ] , and that a linearized description is justified . The microscopic theory of « hydrodynamical modes ... K ̧ ( v % , v ' ) eq - k k1 with ( 6.6 ) q Ро K1 ( v , TOPICS IN NONEQUILIBRIUM STATISTICAL MECHANICS 333 Theory of ...
... exp [ — H / kT ] , and that a linearized description is justified . The microscopic theory of « hydrodynamical modes ... K ̧ ( v % , v ' ) eq - k k1 with ( 6.6 ) q Ро K1 ( v , TOPICS IN NONEQUILIBRIUM STATISTICAL MECHANICS 333 Theory of ...
Page 348
... ( K , F ) whose domain F of definition is in fact a Borel field . Then P is a probability measure exactly if one of ... ( E „ ) = 0 if { E „ } \ ^ [ continuity ] ; ( 2.6 ) if { E } is a countable measurable partition of K and p1 < P ( A / E ...
... ( K , F ) whose domain F of definition is in fact a Borel field . Then P is a probability measure exactly if one of ... ( E „ ) = 0 if { E „ } \ ^ [ continuity ] ; ( 2.6 ) if { E } is a countable measurable partition of K and p1 < P ( A / E ...
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