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1,3,2-二噻唑基自由基中的双稳态

Bistabilities in 1,3,2-dithiazolyl radicals.

作者信息

Brusso Jaclyn L, Clements Owen P, Haddon Robert C, Itkis Mikhail E, Leitch Alicea A, Oakley Richard T, Reed Robert W, Richardson John F

机构信息

Department of Chemistry, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada.

出版信息

J Am Chem Soc. 2004 Jul 7;126(26):8256-65. doi: 10.1021/ja048618m.

Abstract

New synthetic methods for heterocyclic 1,3,2-dithiazolyl (DTA) radicals have been developed, and trends in the molecular spin distributions and electrochemical properties of a series of DTA radicals are reported. The crystal structures of [1,2,5]thiadiazolo[3,4-f][1,3,2]benzodithiazol-2-yl (TBDTA) and [1,3,2]pyrazinodithiazol-2-yl (PDTA) have been determined. The structure of TBDTA (at 293 and 95 K) contains two molecules in the asymmetric unit, each of which generates pi-stacked arrays, one consisting of antiparallel chains of centrosymmetrically associated dimers, the other comprising parallel chains of unassociated radicals. The structure of PDTA (at 293 and 95 K) is simpler, consisting of slipped stacks of pi-dimers. Variable-temperature magnetic susceptibility (chi(P)) measurements on TBDTA indicate essentially paramagnetic behavior for the unassociated radical pi-stacks over the range 5-400 K. By contrast PDTA is diamagnetic at all temperatures below 300 K, but between 300 and 350 K the value of chi(P) follows a sharp and well-defined hysteresis loop, with T(C) downward arrow = 297 K and T(C) upward arrow = 343 K. These features are symptomatic of a regime of bistability involving the observed low temperature pi-dimer structure and a putative high-temperature radical pi-stack. A mechanism for the interconversion of the two phases of PDTA and related structures is proposed in which hysteretic behavior arises from cooperative effects associated with the breaking and making of a lattice-wide network of intermolecular S- - -N' and/or S- - -S' interactions.

摘要

已开发出用于杂环1,3,2 - 二噻唑基(DTA)自由基的新合成方法,并报道了一系列DTA自由基的分子自旋分布和电化学性质趋势。已测定了[1,2,5]噻二唑并[3,4 - f][1,3,2]苯并二噻唑 - 2 - 基(TBDTA)和[1,3,2]吡嗪二噻唑 - 2 - 基(PDTA)的晶体结构。TBDTA(在293 K和95 K)的结构在不对称单元中包含两个分子,每个分子都形成π堆积阵列,一个由中心对称关联二聚体的反平行链组成,另一个由未关联自由基的平行链组成。PDTA(在293 K和95 K)的结构更简单,由π二聚体的滑移堆积组成。对TBDTA进行的变温磁化率(χ(P))测量表明,在5 - 400 K范围内,未关联自由基的π堆积基本表现为顺磁行为。相比之下,PDTA在300 K以下的所有温度下都是抗磁性的,但在300至350 K之间,χ(P)的值遵循一个尖锐且明确的磁滞回线,T(C)向下箭头 = 297 K,T(C)向上箭头 = 343 K。这些特征表明存在一种双稳态势,涉及观察到的低温π二聚体结构和假定的高温自由基π堆积。提出了PDTA两相及相关结构相互转化的机制,其中磁滞行为源于与分子间S - - -N'和/或S - - -S'相互作用的晶格范围网络的断裂和形成相关的协同效应。

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