Brady Clare, Callaghan Philip L, Ciunik Zbigniew, Coates Colin G, Døssing Anders, Hazell Alan, McGarvey John J, Schenker Sabine, Toftlund Hans, Trautwein Alfred X, Winkler Heiner, Wolny Juliusz A
School of Chemistry, Queens University Belfast, Stranmillis Road, Belfast BT9 5AG, Northern Ireland.
Inorg Chem. 2004 Jul 12;43(14):4289-99. doi: 10.1021/ic049809t.
The spin-crossover system Fe(btpa)(2) (btpa = N,N,N',N'-tetrakis(2-pyridylmethyl)-6,6'-bis(aminomethyl)-2,2'-bipyridine) and the predominantly low-spin species Fe(b(bdpa))(2) ((b(bdpa) = N,N'-bis(benzyl)-N,N'-bis(2-pyridylmethyl)-6,6'-bis(aminomethyl)-2,2'-bipyridine) have been characterized by means of X-ray diffraction. The unit cell of Fe(btpa)(2) contains two crystallographically independent molecules revealing octahedral low-spin and quasi-seven-coordinated high-spin structures. The unit cell of Fe(b(bdpa))(2) contains two crystallographically independent molecules one of which corresponds to a low-spin structure, while the other reveals a disordering. On the basis of magnetic susceptibility and Mössbauer measurements, it has been proposed that this disorder involves low-spin and high-spin six-coordinated molecules. The structures of Zn(btpa)(2) and Ru(btpa)(2) have been determined also. Pulsed laser photoperturbation, coupled here with time-resolved resonance Raman spectroscopy (TR(3)), has been used to investigate, for the first time by this technique, the relaxation dynamics in solution on nanosecond and picosecond time scales of low-spin, LS ((1)A) --> high-spin, HS ((5)T) electronic spin-state crossover in these Fe(II) complexes. For the nanosecond experiments, use of a probe wavelength at 321 nm, falling within the pi-pi transition of the polypyridyl backbone of the ligands, enabled the investigation of vibrational modes of both LS and HS isomers, through coupling to spin-state-dependent angle changes of the backbone. Supplementary investigations of the spin-crossover (SCO) equilibrium in homogeneous solution and in colloidal media assisted the assignment of prominent features in the Raman spectra of the LS and HS isomers. The relaxation data from the nanosecond studies confirm and extend earlier spectrophotometric findings, (Schenker, S.; Stein, P. C.; Wolny, J. A.; Brady, C.; McGarvey, J. J.; Toftlund, H.; Hauser, A. Inorg. Chem. 2001, 40, 134), pointing to biphasic spin-state relaxation in the case of Fe(btpa)(2) but monophasic in the case of Fe(b(bdpa))(2). The picosecond results suggest an early process complete in 20 ps or less, which is common to both complexes and possibly includes vibrational relaxation in the initially formed (5)T(2) state.
自旋交叉体系Fe(btpa)₂(btpa = N,N,N',N'-四(2-吡啶甲基)-6,6'-双(氨甲基)-2,2'-联吡啶)以及主要为低自旋态的物种Fe(b(bdpa))₂((b(bdpa) = N,N'-双(苄基)-N,N'-双(2-吡啶甲基)-6,6'-双(氨甲基)-2,2'-联吡啶)已通过X射线衍射进行了表征。Fe(btpa)₂的晶胞包含两个晶体学独立的分子,呈现出八面体低自旋和准七配位高自旋结构。Fe(b(bdpa))₂的晶胞包含两个晶体学独立的分子,其中一个对应低自旋结构,而另一个显示出无序状态。基于磁化率和穆斯堡尔测量结果,有人提出这种无序涉及低自旋和高自旋六配位分子。Zn(btpa)₂和Ru(btpa)₂的结构也已确定。脉冲激光光扰动与时间分辨共振拉曼光谱(TR₃)在此相结合,首次通过该技术研究了这些Fe(II)配合物在纳秒和皮秒时间尺度上低自旋态LS ((¹A))→高自旋态HS ((⁵T))电子自旋态交叉在溶液中的弛豫动力学。对于纳秒实验,使用321 nm的探测波长,该波长落在配体多吡啶主链的π - π跃迁范围内,通过与主链自旋态相关的角度变化耦合,能够研究LS和HS异构体的振动模式。对均相溶液和胶体介质中自旋交叉(SCO)平衡的补充研究有助于确定LS和HS异构体拉曼光谱中的显著特征。纳秒研究的弛豫数据证实并扩展了早期的分光光度法研究结果(申克,S.;斯坦,P. C.;沃尔尼,J. A.;布雷迪,C.;麦加维,J. J.;托夫特伦德,H.;豪泽,A. 《无机化学》2001年,40卷,134页),表明Fe(btpa)₂的自旋态弛豫为双相,而Fe(b(bdpa))₂为单相。皮秒级的结果表明存在一个在20皮秒或更短时间内完成的早期过程,这是两种配合物共有的,并且可能包括最初形成的(⁵T₂)态的振动弛豫。