Proceedings of the International School of Physics "Enrico Fermi.", Volume 72N. Zanichelli, 1979 - Nuclear physics |
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Page 104
... wave function is not complete or 2 ) when the operators corresponding to two ... vector of a system S is an eigenvector « ¿ of a magnitude A , then S has the ... vector x , ) comprises a , and those prop- erties consistent with a ...
... wave function is not complete or 2 ) when the operators corresponding to two ... vector of a system S is an eigenvector « ¿ of a magnitude A , then S has the ... vector x , ) comprises a , and those prop- erties consistent with a ...
Page 335
... wave vector q as a smallness parameter . Assuming that the five frequencies admit an expansion of the form ( 6.11 ) = b ( n ) q + d ( n ) q2 + O ( q2 + e ) , one computes the coefficients b " ) and d ) in terms of the matrix elements of ...
... wave vector q as a smallness parameter . Assuming that the five frequencies admit an expansion of the form ( 6.11 ) = b ( n ) q + d ( n ) q2 + O ( q2 + e ) , one computes the coefficients b " ) and d ) in terms of the matrix elements of ...
Page 336
... wave vector , because in macroscopic hydrodynamics it is assumed that the gradients are weak . It turns out that to O ( q2 ) these moments satisfy a closed set of equations , namely ( we write n , instead of dn , etc. ) ( 6.14a ) iding ...
... wave vector , because in macroscopic hydrodynamics it is assumed that the gradients are weak . It turns out that to O ( q2 ) these moments satisfy a closed set of equations , namely ( we write n , instead of dn , etc. ) ( 6.14a ) iding ...
Contents
The discovery of the law of radioactive decay | 6 |
Early models of the nucleus | 15 |
Final remarks | 21 |
Copyright | |
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