Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 35
... disjoint elements , and every state is additive on disjoint elements , i.e. a ( a \ / b ) = x ( a ) + x ( b ) when a 1 b . With this law the mapping aa becomes an orthocomplementation in : indeed , besides items i ) and ii ) quoted ...
... disjoint elements , and every state is additive on disjoint elements , i.e. a ( a \ / b ) = x ( a ) + x ( b ) when a 1 b . With this law the mapping aa becomes an orthocomplementation in : indeed , besides items i ) and ii ) quoted ...
Page 38
... disjoint , and we write a ) ( b , whenever a b ( but we do not require , now , x ( a ) + x ( b ) < 1 ) . Then it is natural to adopt a law analogous to ( 2.3 ) , namely ( 2.3 ' ) There exists in the join of disjoint elements , and every ...
... disjoint , and we write a ) ( b , whenever a b ( but we do not require , now , x ( a ) + x ( b ) < 1 ) . Then it is natural to adopt a law analogous to ( 2.3 ) , namely ( 2.3 ' ) There exists in the join of disjoint elements , and every ...
Page 127
... disjoint sets , then x ( E1 ) and x ( E , ) are disjoint sets ; iii ) x ( UE ̧ ) = Ụ x ( E , ) if E , is a sequence of disjoint sets . i The probability measure on the real line μ ( x ( E ) ) ( E = B ( R ) ) is called the distri- bution ...
... disjoint sets , then x ( E1 ) and x ( E , ) are disjoint sets ; iii ) x ( UE ̧ ) = Ụ x ( E , ) if E , is a sequence of disjoint sets . i The probability measure on the real line μ ( x ( E ) ) ( E = B ( R ) ) is called the distri- bution ...
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
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