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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Bogomyakov, Artem S.
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article
Heterospin π-heterocyclic radical-anion salt
Abstract
<p>Decamethylchromocene, Cr<sup>II</sup>(η<sup>5</sup>-C <sub>5</sub>(CH<sub>3</sub>)<sub>5</sub>)<sub>2</sub> (2), readily reduced [1,2,5]thiadiazolo[3,4-c][1,2,5]thiadiazole (1) in a tetrahydrofuran solvent at ambient temperature with the formation of radical-anion salt [2] <sup>+</sup>[1]<sup>-</sup> (3) isolated in 97% yield. The heterospin salt 3 ([2]<sup>+</sup>, S = <sup>3</sup>/<sub>2</sub>; [1]<sup>-</sup>, S = <sup>1</sup>/<sub>2</sub>) was characterized by single-crystal X-ray diffraction as well as magnetic susceptibility measurements in the temperature range 2-300 K. The experimental data together with theoretical analysis of the salt-s magnetic structure within the CASSCF and spin-unrestricted broken-symmetry (BS) density functional theory (DFT) approaches revealed antiferromagnetic (AF) interactions in the crystalline 3: significant between anions [1]<sup>-</sup>, weak between cations [2]<sup>+</sup>, and very weak between [1]<sup>-</sup> and [2]<sup>+</sup>. Experimental temperature dependences of the magnetic susceptibility and the effective magnetic moment of 3 were very well reproduced in the assumption of the AF-coupled [1]<sup>-</sup>⋯[1]<sup>-</sup> (J<sub>1</sub> = -40 ± 9 cm<sup>-1</sup>) and [2]<sup>+</sup>⋯ [2]<sup>+</sup> (J<sub>2</sub> = -0.58 ± 0.03 cm<sup>-1</sup>) pairs. The experimental J<sub>1</sub> value is in reasonable agreement with the value calculated using BS UB3LYP/6-31+G(d) (-61 cm<sup>-1</sup>) and CASSCF(10,10)/6-31+G(d) (-15.3 cm<sup>-1</sup>) approaches. The experimental J<sub>2</sub> value is also in agreement with that calculated using the BS DFT approach (-0.33 cm<sup>-1</sup>).</p>