visual-cortex
发表于 2025-3-25 06:27:20
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Disk199
发表于 2025-3-25 11:18:23
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CLAY
发表于 2025-3-25 12:57:29
Strong-Field Couplingmmetric (. — 1)-electron function times a function for the Nth electron. The coefficients of this expansion are the cfp (cf. Section 2.3). The method has been extended by Horie. and others. and may be readily generalized to the problem at hand, i.e., to an arbitrary configuration of inequivalent electron states in an arbitrary point group ..
EWE
发表于 2025-3-25 16:20:16
hese diagrams are limited in scope in that they can be used only for octahedral symmetry and for a limited number of terms. The present volume is an attempt to fill the gap by providing a reasonable nurober of complete and accurate ligand field energy diagrarns for dN configurations in the most comm
就职
发表于 2025-3-25 21:54:49
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Grandstand
发表于 2025-3-26 00:48:26
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Basal-Ganglia
发表于 2025-3-26 05:43:32
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Creditee
发表于 2025-3-26 09:12:52
Tensor Operator Algebra in Free Atoms and Ionsl harmonics .. = |.〉 then arise in a natural way as the simultaneous eigenfunctions of the Hamiltonian and the operators .. and .. of the square of the total angular momentum and of its . component. This fact is intimately related to the transformation properties of the |.〉 eigenvectors under rotati
capillaries
发表于 2025-3-26 12:40:36
Weak-Field Couplingre . = ., .−1,..., −. (cf. Section 2.4). The effect of a ligand field of particular symmetry consists, in general, in splitting the free ion levels labeled by . into ligand field states. The decomposition is equivalent to the reduction .where ..(.) is subduced from representation .. of .(3) and wher
Aviary
发表于 2025-3-26 20:21:35
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