...
首页> 外文期刊>European journal of inorganic chemistry >Two-step versus one-step spin transitions in iron(II) 1D chain compounds
【24h】

Two-step versus one-step spin transitions in iron(II) 1D chain compounds

机译:铁(II)1D链化合物的两步自旋转变与一步自旋转变

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

Eleven iron(II) 1D coordination polymers with the general formula [FeL _(eq)(L_(ax))]·solvent were synthesised and characterised, where L_(eq) = (E,E)-{diethyl 2,2′-[1,2- phenylenebis(iminomethylidyne)]bis(3-oxobutanato) (2-)-N,N′,O ~3,O~(3′)} (L1) and {[3,3′]-[1,2- phenylenebis(iminomethylidyne)]bis(2,4-pentane-dionato)(2-)-N,N′,O ~2,O~(2′)} (L2); L_(ax) = 4,4′-bipyridine (bipy), 1,2-bis(4-pyridyl)ethane (bpea) and 1,3-bis(4-pyridyl)propane (bppa) and solvent = MeOH, EtOH and toluene (Tol). [FeL1(bpea)]·MeOH (3·MeOH) shows an abrupt one-step spin crossover with thermal hysteresis(27 K) and [FeL2(bppa)]·MeOH (2·MeOH), [FeL2(bpea)] (4), [FeL2(bpea)]·0.25MeOH (4·0.25MeOH) and [FeL1(bipy)]·MeOH (5·MeOH) show a two-step spin transition with an IP at γ_(HS) ≈ 0.5 (IP is intermediate plateau and γHS is high-spin mol fraction) and up to 50 K wide hysteresis loops (5·MeOH). [FeL1(bppa)] (1), [FeL2(bppa)]·EtOH (2·EtOH) and [FeL1(bpea)]·1.5Tol (3·1.5Tol) show an abrupt incomplete spin transition that stops at γ_(HS) ≈ 0.5; for [FeL1(bppa)]·0.25MeOH (1·0.25MeOH) and [FeL1(bpea)] (3), the spin transition is gradual and incomplete. The X-ray crystal structures of six complexes were determined (1, 2·MeOH, 3·MeOH, 3·1.5Tol, 4·0.25MeOH and 5·MeOH). In the case of 4·0.25MeOH, the crystal structures for the HS and LS states were dertermined; for compounds 1, 2·MeOH and 3·1.5Tol, the crystal structure of the HS and the IP state was investigated. For all complexes, the iron(II) centre is located in a distorted octahedral coordination sphere. Each axially coordinated ligand "connects" two iron(II) centres, which results in the formation of extended 1D chains with varying structures from linear (bipy) over steplike (bpea) to zigzag (bppa). Analysis of the intermolecular interactions reveals that the hysteresis width depends on both the stiffness of the axial ligand and the number of intermolecular contacts, while zigzag chains support stepwise spin transitions.
机译:合成并表征了11种通式为[FeL _(eq)(L_(ax))·溶剂的铁(II)一维配位聚合物,其中L_(eq)=(E,E)-{diethyl 2,2' -[[1,2-亚苯基双(亚氨基亚甲基二炔)]双(3-氧代丁酸)(2-)-N,N',O〜3,O〜(3')}(L1)和{[3,3']- [1,2-亚苯基双(亚氨基亚甲基二炔)]双(2,4-戊烷-二酮基)(2-)-N,N',O〜2,O〜(2')}(L2); L_(ax)= 4,4'-联吡啶(bipy),1,2-双(4-吡啶基)乙烷(bpea)和1,3-双(4-吡啶基)丙烷(bppa),溶剂= MeOH,EtOH和甲苯(Tol)。 [FeL1(bpea)]·MeOH(3·MeOH)表现出突然的单步自旋交变,具有热滞(27 K)和[FeL2(bppa)]·MeOH(2·MeOH),[FeL2(bpea)]( 4),[FeL2(bpea)]·0.25MeOH(4·0.25MeOH)和[FeL1(bipy)]·MeOH(5·MeOH)表现出两步自旋转变,其IP在γ_(HS)≈0.5( IP为中等水平,γHS为高自旋摩尔分数),并具有高达50 K的迟滞回线(5·MeOH)。 [FeL1(bppa)](1),[FeL2(bppa)]·EtOH(2·EtOH)和[FeL1(bpea)]·1.5Tol(3·1.5Tol)显示突然的不完全自旋转变,其终止于γ_( HS)≈0.5;对于[FeL1(bppa)]·0.25MeOH(1·0.25MeOH)和[FeL1(bpea)](3),自旋转变是渐进且不完全的。确定了六个配合物的X射线晶体结构(1、2·MeOH,3·MeOH,3·1.5Tol,4·0.25MeOH和5·MeOH)。在4·0.25MeOH的情况下,确定了HS和LS态的晶体结构。对于化合物1、2·MeOH和3·1.5Tol,研究了HS的晶体结构和IP状态。对于所有配合物,铁(II)中心都位于扭曲的八面体配位范围内。每个轴向配位的配体“连接”两个铁(II)中心,这导致形成扩展的一维链,其结构从线性(双联)到阶梯状(bpea)到之字形(bppa)不等。分子间相互作用的分析表明,磁滞宽度取决于轴向配体的刚度和分子间接触的数量,而之字形链则支持逐步的自旋跃迁。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号