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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

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