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Dynamical effects on the magnetic properties of dithiazolyl bistable materials

机译:动力学对双噻唑双稳态材料磁性的影响

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摘要

The magnetic properties of molecule-based magnets are commonly rationalized by considering only a single nuclear configuration of the system under study (usually an X-ray crystal structure). Here, by means of a computational study, we compare the results obtained using such a static approach with those obtained by explicitly accounting for thermal fluctuations, and uncover the serious limitations of the static perspective when dealing with magnetic crystals whose radicals undergo wide-amplitude motions. As a proof of concept, these limitations are illustrated for the magnetically bistable 1,3,5-trithia-2,4,6-triazapentalenyl (TTTA) material. For its high-temperature phase at 300 K, we show that nuclear dynamics induce large fluctuations in the magnetic exchange interactions (J AB) between spins (up to 1000% of the average value). These deviations result in a ∼20% difference between the 300 K magnetic susceptibility computed by explicitly considering the nuclear dynamics and that computed using the X-ray structure, the former being in better agreement with the experimental data. The unveiled strong coupling between J AB interactions and intermolecular vibrations reveals that considering J AB as a constant value at a given temperature (as always done in molecular magnetism) leads to a flawed description of the magnetism of TTTA. Instead, the physically relevant concept in this case is the statistical distribution of J AB values. The discovery that a single X-ray structure is not adequate enough to interpret the magnetic properties of TTTA is also expected to be decisive in other organic magnets with dominant exchange interactions propagating through labile π–π networks.
机译:通常,仅考虑被研究系统的单个核构型(通常是X射线晶体结构)来合理化基于分子的磁体的磁性能。在这里,通过计算研究,我们将使用这种静态方法获得的结果与通过显式考虑热波动获得的结果进行比较,并发现当处理原子团经历宽幅运动的磁性晶体时,静态视角的严重局限性。作为概念的证明,这些局限性是针对磁性双稳态的1,3,5-trithia-2,4,6-三氮杂戊烯基(TTTA)材料。对于300 K的高温相,我们表明核动力学在自旋之间的磁交换相互作用(J AB)中引起了很大的波动(高达平均值的1000%)。这些偏差导致通过明确考虑核动力学计算出的300 K磁化率与使用X射线结构计算出的300 K磁化率之间有约20%的差异,前者与实验数据更好地吻合。 J AB相互作用和分子间振动之间的强相互作用揭示了将J AB作为给定温度下的恒定值(在分子磁性中总是如此)会导致对TTTA磁性的描述存在缺陷。相反,在这种情况下,与物理相关的概念是J AB值的统计分布。单个X射线结构不足以解释TTTA的磁性的发现也有望在其他有机磁体中具有决定性的作用,这些有机磁体具有通过不稳定的π-π网络传播的主要交换相互作用。

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