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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 a-phase crystallizes in the tetragonal space group P42_1m and consists of π-stacked radicals, tightly clustered about 4 points and running parallel to c. The β-phase belongs to the monoclinic space group P2_1/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 x measurements confirm that α-1a behaves as a Curie-Weiss paramagnet; the low-temperature variations in x can be modeled in terms of a 1D Heisenberg chain of weakly coupled AFM S = 1/2 centers. The dimeric phase β-a is essentially diamagnetic up to 380 K. Above this temperature there is a sharp hysteretic (T↑= 380 K, T↓ = 375 K) increase in x and xT. 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 a-bond in α-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。 a相在四方空间群P42_1m中结晶,并由π堆积的自由基组成,紧密聚集约4个点,且平行于c。 β相属于单斜空间群P2_1 / c,在环境温度和压力下,由π堆叠的二聚体组成,其中自由基通过超价四中心六电子S…SS…Sσ-横向连接。债券。可变温度磁化率x的测量结果证实α-1a表现为居里-魏斯顺磁性; x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-a在380 K以下基本上是反磁性的。在该温度以上,x和xT急剧增加磁滞(T↑= 380 K,T↓= 375 K)。 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键断裂。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σRT从0.5 GPa时的10〜(-7)S cm〜(-1)附近增加到10〜( -4)S cm〜(-1)在5 GPa下。 β-1a的σRT值(在0.5 GPa时接近10〜(-4)S cm〜(-1))随着相变的发生而随着压力的增加而减小,但超过1.5 GPa时,这种趋势发生逆转,σRT的值在一种类似于α-1a行为的方式。 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。将α-1a中S…S-S…S a键对热和压力的响应与具有S…Se-Se…Sσ键的相关二聚体的响应进行了比较。

著录项

  • 来源
    《Journal of the 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 SGI, Canada;

    Department of Chemistry, University of Waterloo, Waterloo, Ontario N2L SGI, Canada;

    Department of Physics, University of Ottawa, Ottawa, Ontario KIN 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;

    Department of Physics, University of Ottawa, Ottawa, Ontario KIN 6N5, Canada;

    Department of Earth Sciences, University of Western Ontario, London, Ontario N6A 5B7, Canada;

    Brockhouse Institute for Materials Research, McMaster University, Hamilton, Ontario L8S 4MI, Canada;

    Department of Chemistry, University of Waterloo, Waterloo, Ontario N2L SGI, 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 03:15:57

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