Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 347
... limit P , ( { q } ) = 0 n∞ : limit P1 ( K ) = 1 , n - ∞ for all q in K , K = U { { q } : q = K - a countable union . Hence the defined limit is not a countably additive function . ( This example of additive functions defined on the ...
... limit P , ( { q } ) = 0 n∞ : limit P1 ( K ) = 1 , n - ∞ for all q in K , K = U { { q } : q = K - a countable union . Hence the defined limit is not a countably additive function . ( This example of additive functions defined on the ...
Page 354
... limit as n increases in- definitely . The domain of definition of the set function relf ( — , σ ) is given only in this way . We now turn to the question whether soundness or completeness could be claimed for the probability axioms thus ...
... limit as n increases in- definitely . The domain of definition of the set function relf ( — , σ ) is given only in this way . We now turn to the question whether soundness or completeness could be claimed for the probability axioms thus ...
Page 379
... limit = limit rel ( a , n ) + a ( n ) ' where ba is the characteristic function of AB , namely ba ( n ) = b ( n ) a ( n ) . What I would like to show now is that the natural frequency space is already closed under conditionalization ...
... limit = limit rel ( a , n ) + a ( n ) ' where ba is the characteristic function of AB , namely ba ( n ) = b ( n ) a ( n ) . What I would like to show now is that the natural frequency space is already closed under conditionalization ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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