Anthony KERMAGORET - THESES ET MEMOIRES DE L'UDS
Anthony KERMAGORET - THESES ET MEMOIRES DE L'UDS
Anthony KERMAGORET - THESES ET MEMOIRES DE L'UDS
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Chapitre III<br />
Considering the spin topology described in Figure S-5 and assuming each pairwise<br />
interaction is describable in terms of the Heisenberg Hamiltonian of the form Ĥ = -Jij Ŝi⋅Ŝj, the<br />
complete spin Hamiltonian for Ni4 is given in eq. 1<br />
Ĥ = -J1 Ŝ1⋅Ŝ2 - J2 Ŝ1⋅Ŝ4 - J3Ŝ1⋅Ŝ3 - J2 Ŝ2⋅Ŝ3 - J1 Ŝ3⋅Ŝ4 (1)<br />
As explained by Griffith and by Hendrickson, the existence of three different exchange<br />
constants for this peculiar spin topology prevents the use of the Kambe vector-coupling<br />
[S ,S ,S ]<br />
approach. 4 5 6 Unfortunately, in the present case, no analytical fitting by full diagonalization of<br />
the complete spin Hamiltonian was successful in the whole temperature range. This may infirm the<br />
hypothesis of Heisenberg type interactions.<br />
The magnetic properties of this compound require further studies, for instance by neutron<br />
diffraction, neutron scattering, or high-field EPR spectroscopy, in order to precise the amplitude and<br />
sign of the different exchange constants and the characteristics of the ground state (spin value,<br />
anisotropy).<br />
5. Crystallographic<br />
5.1 X-ray data collection, structure solution and refinement for 1a⋅2CH2Cl2, 3 and 4.<br />
Suitable crystals for X-ray analysis of compounds 1a⋅2CH2Cl2, 3 and 4 were obtained by<br />
layering hexane on dichloromethane solutions. The intensity data was collected at 173(2) K on a<br />
[S- ]<br />
Kappa CCD diffractometer 7 (graphite monochromated MoKα radiation, λ = 0.71073 Å).<br />
Crystallographic and experimental details for the structures are summarized in Table S-1. The<br />
structures were solved by direct methods (SHELXS-97) and refined by full-matrix least-squares<br />
procedures (based on F 2 [S- ]<br />
, SHELXL-97) 8 with anisotropic thermal parameters for all the non-<br />
hydrogen atoms. The hydrogen atoms were introduced into the geometrically calculated positions<br />
and refined riding on the corresponding parent atoms. For 1a, C2 and C6 were found disordered in<br />
two positions with equal occupancy factors and their position was refined isotropically. CCDC-<br />
641489 (3), 641490 (4) and 641491 (1a⋅2CH2Cl2) contain the supplementary crystallographic data<br />
that can be obtained free of charge via www.ccdc.cam.ac.uk/conts/retrieving.html (or from the<br />
Cambridge Crystallographic Data Centre, 12 Union Road, Cambridge CB2 1EZ, UK; fax<br />
(+44)1223-336-033 or deposit@ccdc.cam.ac.uk). Figure 1 was produced using the UCSF Chimera<br />
package from the Computer Graphics Laboratory, University of California, San Francisco: C.C.<br />
Huang, G.S. Couch, E.F. Pettersen, T.E. Ferrin, "Chimera: An Extensible Molecular Modeling<br />
18