Journal of Research of the National Bureau of Standards, Volume 86U.S. Department of Commerce, National Bureau of Standards, 1981 |
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Page 33
... corrections , of the atomic number . There was general qualitative agreement between the values of the parameters calculated using the semi - empirical method and those calculated using Hartree - Fock methods . There remained some ...
... corrections , of the atomic number . There was general qualitative agreement between the values of the parameters calculated using the semi - empirical method and those calculated using Hartree - Fock methods . There remained some ...
Page 34
... corrected values of the parameters including their statistical deviations and the sum of the squares of the differences between the observed and the calculated levels , were obtained . The rms error is then defined as n A = Σ ΔΙ i = 1 n ...
... corrected values of the parameters including their statistical deviations and the sum of the squares of the differences between the observed and the calculated levels , were obtained . The rms error is then defined as n A = Σ ΔΙ i = 1 n ...
Page 35
... correction of this kind for the configurations d was the aL ( L + 1 ) correction introduced by Trees , [ 19-20 ] , in the configurations 3d4s of MnII and FeIII . Trees introduced his correction empirically , but Racah , [ 21 ] , showed ...
... correction of this kind for the configurations d was the aL ( L + 1 ) correction introduced by Trees , [ 19-20 ] , in the configurations 3d4s of MnII and FeIII . Trees introduced his correction empirically , but Racah , [ 21 ] , showed ...
Page 36
... correction term W2 , that must be added to the Hamiltonian of " caused by the perturbation of " by " -1 l'configura- tions is given by where and W2 = - Σ P ( kk ' ; ll , ll ' ) & ( kk ' ; ll , ll ' ) P ( kk ' ; lalo , lold ) = X ( k ...
... correction term W2 , that must be added to the Hamiltonian of " caused by the perturbation of " by " -1 l'configura- tions is given by where and W2 = - Σ P ( kk ' ; ll , ll ' ) & ( kk ' ; ll , ll ' ) P ( kk ' ; lalo , lold ) = X ( k ...
Page 41
... correction . T , T ' , T " parameters of the three - body effective T. , T. , T interactions of the core d ... corrections of n for the configurations ( 3d + 4s ) " in the second spec- tra of the iron group . Now in d " p we must ...
... correction . T , T ' , T " parameters of the three - body effective T. , T. , T interactions of the core d ... corrections of n for the configurations ( 3d + 4s ) " in the second spec- tra of the iron group . Now in d " p we must ...
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