Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 76
... eigenvalue b , of B as well as the choice of basis in the sub- space . In effect , a measurement of B is regarded as a measurement of some maximal magnitude A , such that B = f ( A ) , with loss of information . Thus , the measurement ...
... eigenvalue b , of B as well as the choice of basis in the sub- space . In effect , a measurement of B is regarded as a measurement of some maximal magnitude A , such that B = f ( A ) , with loss of information . Thus , the measurement ...
Page 182
... eigenvalue r , and by the ( normalized ) eigen- vector of g ( Q ) with eigenvalue r ,, which means : i with certainty the value for Q ; in y could be r , or the value for Q , in could be r¡ . In other words , the quantum - logical ...
... eigenvalue r , and by the ( normalized ) eigen- vector of g ( Q ) with eigenvalue r ,, which means : i with certainty the value for Q ; in y could be r , or the value for Q , in could be r¡ . In other words , the quantum - logical ...
Page 268
... eigenvalues 0 and 1. Therefore , it may be considered as an observable with measuring values 0 and 1. If a quantum- mechanical system is described by a state vector Є H , the equation PAY ( eigenvalue 1 ) means that pe A , and the ...
... eigenvalues 0 and 1. Therefore , it may be considered as an observable with measuring values 0 and 1. If a quantum- mechanical system is described by a state vector Є H , the equation PAY ( eigenvalue 1 ) means that pe A , and the ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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