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This paper is devoted to the determination of the spin distribution in the spin triplet ground state of [Cu 2 ( t -Bupy) 4 (N 3 ) 2 ](ClO 4 ) 2, with t -Bupy = p - tert -butylpyridine. The crystal structure, previously solved at room temperature from X-ray diffraction, has been redetermined at 18 K from unpolarized neutron diffraction. The structure consists of binuclear cations in which Cu 2+ ions are doubly bridged by azido groups in the 1,1-fashion, and noncoordinated perchlorate anions. The experimental spin distribution has been determined from polarized neutron diffraction (PND) at 1.6 K under 50 kOe. The spin populations have been found to be strongly positive on the Cu 2+ ions, weakly positive on the terminal and bridging nitrogen atoms of the azido groups as well as on the nitrogen atoms of the t -Bupy ligands, and weakly negative on the central nitrogen atoms of the N 3 - bridges. The PND results have been discussed. The spin distribution in [Cu 2 ( t -Bupy) 4 (N 3 ) 2 ](ClO 4 ) 2 has been analyzed as resulting from a spin delocalization from the Cu 2+ ions toward the azido bridges, to which a spin polarization effect within the azido π orbitals is superimposed. The experimental data have been compared to the results of DFT calculations. The spin density map is qualitatively reproduced; however, the DFT calculations overestimate the spin delocalization from the Cu 2+ ions toward the peripheral and bridging ligands.
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Aebersold et al. (1998) studied this question.
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