1997
DOI: 10.1016/s0301-0104(97)00042-6
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Nature of the magnetic interaction of Wurster's radicals in the solid state

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Cited by 16 publications
(20 citation statements)
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“…∆ depends on the topology and the geometry of the stacks: ∆ is zero (or has small values) in the case of models of class (i); ∆ has finite values which increase with increasing slip angle R. Quantitatively, the same conclusion was drawn from theoretical investigations of the nature of the magnetic interaction of Wurster's radicals in the solid state. 16 The intermolecular magnetic coupling within the MRCs is 1 order of magnitude smaller in comparison with the intramo-lecular magnetic coupling between galvinoxyl radicals connected by meta-phenylene units in an 1-D polymer.…”
Section: Discussionmentioning
confidence: 94%
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“…∆ depends on the topology and the geometry of the stacks: ∆ is zero (or has small values) in the case of models of class (i); ∆ has finite values which increase with increasing slip angle R. Quantitatively, the same conclusion was drawn from theoretical investigations of the nature of the magnetic interaction of Wurster's radicals in the solid state. 16 The intermolecular magnetic coupling within the MRCs is 1 order of magnitude smaller in comparison with the intramo-lecular magnetic coupling between galvinoxyl radicals connected by meta-phenylene units in an 1-D polymer.…”
Section: Discussionmentioning
confidence: 94%
“…In contrast to galvinoxyl MRCs, the magnitude of the magnetic interaction (antiferromagnetic in nature) between neighboring Wurster's radicals in the 1-D stacks of Wurster's Red Bromide is large, J eff ∼ 0.1 eV. 16 This relative large absolute value of J eff is caused by the short interplanar distance between the Wurster's radicals in the stacks (R(exp) ) 3.105 Å 22 ).…”
Section: Resultsmentioning
confidence: 99%
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“…Thus homo-radical stacks (Scheme 1a) are likely to exhibit anti-parallel spin alignment and zero net collective spin, as shown for neutral and charged Wurster-type radicals. 14,15 If a diamagnetic molecule (N) is inserted between each pair of radicals in the stack, its spin polarisation (SP), albeit weak, can lead to an effective ferrimagnetic ordering with the large spin-up/down densities on the radicals and small (induced) spin-down/-up density on the spacers (Scheme 1b).…”
Section: Introductionmentioning
confidence: 99%