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Ensemble‐representable densities for atoms and molecules. II. Application to CoCl 4 2−
Author(s) -
CassamChenaï P.,
Wolff S. K.,
Chandler G. S.,
Figgis B. N.
Publication year - 1996
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/(sici)1097-461x(1996)60:2<667::aid-qua5>3.0.co;2-v
Subject(s) - diamagnetism , magnetization , collinearity , paramagnetism , physics , constraint (computer aided design) , statistical physics , crystal (programming language) , spin (aerodynamics) , neutron diffraction , interpretation (philosophy) , magnetic field , diffraction , condensed matter physics , quantum mechanics , mathematics , computer science , thermodynamics , statistics , geometry , programming language
In the previous article we introduced a method to obtain an ensemble density describing a molecule in a crystal from diffraction experiment structure factors. Here the method is applied to the CoCl 4 2− molecular ion in a Cs 3 CoCl 5 crystal for which accurate magnetic structure factors are known. First, the approximations involved in the interpretation of polarized neutron experiment are reviewed with special emphasis on the collinearity approximation which has been avoided in this work. Second, the derivation of magnetic structure factors corresponding to theoretical ensemble densities is explained (the spin and the exact orbital contributions have been included). Third, the fitting procedure is presented and results at different levels of approximation are discussed. The main conclusions are: (1) A density built by using several molecular wave functions can give a very good agreement with the experimental data. (2) The ensemble representability constraint is necessary to retrieve physical information from the optimized parameters. (3) Taking into account the proper paramagnetic contribution to the magnetization improves significantly the agreement between theory and experiment. (4) Neglecting the diamagnetic contribution and the fact that the magnetization may be locally noncollinear to the applied external field is fully justified for the system under study. © 1996 John Wiley & Sons, Inc.