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The latter trend may be caused by an admixture of dimers or by intermolecular interactions . ... Another superexchange channel can be represented by the stacking interaction between the planes of chelate cycles , which are spaced by 3.6 ...
The latter trend may be caused by an admixture of dimers or by intermolecular interactions . ... Another superexchange channel can be represented by the stacking interaction between the planes of chelate cycles , which are spaced by 3.6 ...
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S - = = 2 2 + XZ 2 8 = = For the anisotropic spin - orbit interaction constant , ( Eyz - E ) a + ( 4 , / 2 ) b + ( 4 , / 2 ) c = 0 ; ( 4 , / 2 ) a + ( Ex - E ) b + ( 4_ / 2 ) c = 0 ; ( 11/2 ) a + ( 11/2 ) b + ( Ex ; – E ) c = 0 ...
S - = = 2 2 + XZ 2 8 = = For the anisotropic spin - orbit interaction constant , ( Eyz - E ) a + ( 4 , / 2 ) b + ( 4 , / 2 ) c = 0 ; ( 4 , / 2 ) a + ( Ex - E ) b + ( 4_ / 2 ) c = 0 ; ( 11/2 ) a + ( 11/2 ) b + ( Ex ; – E ) c = 0 ...
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Interaction kinetics in the system 2 ( 1 – x ) S CO3 + 2xCuO + Nb205 ( 850 ° C ) : ( 1 ) x = 0 , ( 2 ) 0.1 , ( 3 ) 0.2 . The lines are theoretical curves for limiting stages : ( A ) nucleation ; ( R ) direct chemical interaction ...
Interaction kinetics in the system 2 ( 1 – x ) S CO3 + 2xCuO + Nb205 ( 850 ° C ) : ( 1 ) x = 0 , ( 2 ) 0.1 , ( 3 ) 0.2 . The lines are theoretical curves for limiting stages : ( A ) nucleation ; ( R ) direct chemical interaction ...
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