Létard Jean-François, Carbonera Chiara, Real José Antonio, Kawata Satoshi, Kaizaki Sumio
ICMCB, CNRS, Université Bordeaux, Groupe des Sciences Moléculaires, 87 Av. Doc. A. Schweitzer, 33608 Pessac, France.
Chemistry. 2009;15(16):4146-55. doi: 10.1002/chem.200802171.
Spin crossover: The photomagnetic properties of a series of [{Fe(NCS)(py-X)}(2)(bpypz)(2)] (NCS=thiocyanate, py=pyridine, X=4-Mepy, py, 3-Mepy, 3-Clpy and 3-Brpy, and bpypz=3,5-bis(pyridine-2-yl)pyazolate) binuclear complexes are close to the antiferromagnetic response of [{Fe(NCS)(3,5-dmpy)}(3)(bpypz)(2)] (3,5-dmpy=3,5-dimethylpyrazine), which is characterised by two iron(II) metal ions in a high-spin (HS) electronic configuration (see figure).This paper describes the photomagnetic properties of a series of binuclear iron(II) complexes belonging to the [{Fe(NCS)(py-X)}(2)(bpypz)(2)] family (NCS=thiocyanate; py=pyridine; bpypz=3,5-bis(pyridine-2-yl)pyrazolate; and py-X=4-Mepy (1), py (3), 3-Mepy (4), 3-Clpy (5), and 3-Brpy (6)). All of these complexes display a complete thermal spin transition centred between 100 and 150 K, and undergo the light-induced excited-spin-state trapping (LIESST) effect at low temperatures. The T(LIESST) relaxation temperature of the photoinduced high-spin state for each compound has been determined. For all of the complexes, it has been found that the T(LIESST) curves at low temperature are close to the antiferromagnetic response of the [{Fe(NCS)(3,5-dmpy)}(2)(bpypz)(2)] (3,5-dmpy=3,5-dimethylpyridine) (7) complex that is characterised by two iron(II) metal ions in a HS electronic configuration, giving some evidence of a quantitative low spin-low spin-->high spin-high spin (LS-LS-->HS-HS) photoconversion process. Depending on the nature of the cooperativity, the kinetics have been treated with stretched exponential, simply exponential, or sigmoidal models. Interestingly, this series of dinuclear complexes follows a previously proposed linear relationship between the T(LIESST) and their thermal spin transition temperatures T(1/2): T(LIESST)=T(0)-0.3T(1/2). T(0) for these compounds is equal to 100 K. Based on this, and by using the empirical linear relationship found between the thermal spin transition and the Hammett constant, the HS-HS properties of complex 7 have been understood as a reflection of the physical impossibility that the T(LIESST) was higher than T(1/2). The close vicinity of the thermal spin-crossover phenomenon of 7 has been successfully checked by applying hydrostatic pressure.
一系列[{Fe(NCS)(py-X)}(2)(bpypz)(2)](NCS =硫氰酸盐,py =吡啶,X = 4-甲基吡啶、吡啶、3-甲基吡啶、3-氯吡啶和3-溴吡啶,且bpypz = 3,5-双(吡啶-2-基)吡唑盐)双核配合物的光磁性质接近于[{Fe(NCS)(3,5-二甲基吡啶)}(3)(bpypz)(2)](3,5-二甲基吡啶= 3,5-二甲基吡嗪)的反铁磁响应,其特征是两个铁(II)金属离子处于高自旋(HS)电子构型(见图)。本文描述了属于[{Fe(NCS)(py-X)}(2)(bpypz)(2)]家族的一系列双核铁(II)配合物的光磁性质(NCS =硫氰酸盐;py =吡啶;bpypz = 3,5-双(吡啶-2-基)吡唑盐;且py-X = 4-甲基吡啶(1)、吡啶(3)、3-甲基吡啶(4)、3-氯吡啶(5)和3-溴吡啶(6))。所有这些配合物在100至150 K之间均表现出完全的热自旋转变,并在低温下经历光诱导激发自旋态俘获(LIESST)效应。已测定了每种化合物光诱导高自旋态的T(LIESST)弛豫温度。对于所有配合物,已发现低温下的T(LIESST)曲线接近于[{Fe(NCS)(3,5-二甲基吡啶)}(2)(bpypz)(2)](3,5-二甲基吡啶= 3,5-二甲基吡啶)(7)配合物的反铁磁响应,其特征是两个铁(II)金属离子处于HS电子构型,这为定量的低自旋-低自旋→高自旋-高自旋(LS-LS→HS-HS)光转换过程提供了一些证据。根据协同性的性质,动力学已用拉伸指数、简单指数或S形模型进行处理。有趣的是,这一系列双核配合物遵循先前提出的T(LIESST)与其热自旋转变温度T(1/2)之间的线性关系:T(LIESST)=T(0)-0.3T(1/2)。这些化合物的T(0)等于100 K。基于此,并通过利用热自旋转变与哈米特常数之间发现的经验线性关系,配合物7的HS-HS性质被理解为T(LIESST)高于T(1/2)这一物理上不可能情况的反映。通过施加静水压力已成功验证了配合物7热自旋交叉现象的紧密关联性。