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Hysteretic Spin Crossover between a Bisdithiazolyl Radical and Its Hypervalent σ-Dimer

机译:Bisdithiazolyl自由基与其超价σ-Dimer之间的磁滞自旋交叉

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摘要

The bisdithiazolyl radical 1a is dimorphic, existing in two distinct molecular and crystal modifications. The α-phase crystallizes in the tetragonal space group P4̅21m and consists of π-stacked radicals, tightly clustered about 4̅ points and running parallel to c. The β-phase belongs to the monoclinic space group P21/c and, at ambient temperature and pressure, is composed of π-stacked dimers in which the radicals are linked laterally by hypervalent four-center six-electron S···S−S···S σ-bonds. Variable-temperature magnetic susceptibility χ measurements confirm that α-1a behaves as a Curie−Weiss paramagnet; the low-temperature variations in χ can be modeled in terms of a 1D Heisenberg chain of weakly coupled AFM S = 1/2 centers. The dimeric phase β-1a is essentially diamagnetic up to 380 K. Above this temperature there is a sharp hysteretic (T↑= 380 K, T↓ = 375 K) increase in χ and χT. Powder X-ray diffraction analysis of β-1a at 393 K has established that the phase transition corresponds to a dimer-to-radical conversion in which the hypervalent S···S−S···S σ-bond is cleaved. Variable-temperature and -pressure conductivity measurements indicate that α-1a behaves as a Mott insulator, but the ambient-temperature conductivity σRT increases from near 10−7 S cm−1 at 0.5 GPa to near 10−4 S cm−1 at 5 GPa. The value of σRT for β-1a (near 10−4 S cm−1 at 0.5 GPa) initially decreases with pressure as the phase change takes place, but beyond 1.5 GPa this trend reverses, and σRT increases in a manner which parallels the behavior of α-1a. These changes in conductivity of β-1a are interpreted in terms of a pressure-induced dimer-to-radical phase change. High-pressure, ambient-temperature powder diffraction analysis of β-1a confirms such a transition between 0.65 and 0.98 GPa and establishes that the structural change involves rupture of the dimer in a manner akin to that observed at high temperature and ambient pressure. The response of the S···S−S···S σ-bond in β-1a to heat and pressure is compared to that of related dimers possessing S···Se−Se···S σ-bonds.
机译:双二噻唑基1a是双晶的,以两种不同的分子和晶体修饰形式存在。 α相在四方空间群P4̅2 1 m中结晶,由π堆积的基团组成,紧密簇集约4̅点,并平行于c延伸。 β相属于单斜晶空间群P2 1 / c,在环境温度和压力下,它由π堆叠的二聚体组成,其中自由基通过超价四中心六键横向连接。电子S···S····Sσ键。可变温度磁化率χ值测量证实α-1a表现为居里·魏斯顺磁体。 χ的低温变化可以用弱耦合AFM S = 1 / 2 中心的一维Heisenberg链建模。二聚体相β-1a在最高380 K时基本上是反磁性的。在该温度以上,χ和χT出现明显的磁滞(T↑= 380 K,T↓= 375 K)增加。 β-1a在393 K的粉末X射线衍射分析表明,相变对应于二聚体到自由基的转化,其中高价S···S·S···Sσ键被裂解。可变温度和压力电导率测量表明,α-1a表现为莫特绝缘子,但环境温度电导率σ RT 从接近10 −7 S cm <在0.5 GPa时sup> -1 到在5 GPa时接近10 -4 S cm -1 。 β-1a的σ RT 值(在0.5 GPa下接近10 −4 S cm −1 )最初随着压力的减小而减小发生了变化,但超过1.5 GPa时,这种趋势发生了逆转,并且σ RT 以与α-1a行为相似的方式增加。 β-1a电导率的这些变化是根据压力引起的二聚体到自由基相变来解释的。 β-1a的高压,常温粉末衍射分析证实了0.65至0.98 GPa之间的这种转变,并确定了结构变化涉及二聚体的破裂,其方式类似于在高温和环境压力下观察到的方式。比较了β-1a中S··S·S···Sσ键对热和压力的响应与相关的具有S··Se·Se··Sσ键的二聚体的响应。

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  • 来源
    《American Chemical Society》 |2010年第45期|p.16212-16224|共13页
  • 作者单位

    Department of Chemistry, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada, Department of Physics, University of Ottawa, Ottawa, Ontario K1N 6N5, Canada, Department of Earth Sciences, University of Western Ontario, London, Ontario N6A 5B7, Canada, Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, Saskatchewan S7N 5E2, Canada, and Brockhouse Institute for Materials Research, McMaster University, Hamilton, Ontario L8S 4M1, Canada;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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  • 正文语种 eng
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  • 入库时间 2022-08-18 00:50:26

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