首页> 外文期刊>ACS Omega >{CpFeII(CO)2SnII(Macrocycle?3?)} Radicals with Intrinsic ChargeTransfer from CpFe(CO)2 to Macrocycles (Cp: Cp or Cp*); EffectiveMagnetic Coupling between Radical Trianionic Macrocycles?3?
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{CpFeII(CO)2SnII(Macrocycle?3?)} Radicals with Intrinsic ChargeTransfer from CpFe(CO)2 to Macrocycles (Cp: Cp or Cp*); EffectiveMagnetic Coupling between Radical Trianionic Macrocycles?3?

机译:{CpFeII(CO)2SnII(Macrocycle?3?)}具有从CpFe(CO)2到大环(Cp:Cp或Cp *)的固有电荷转移的基团;自由基三阴离子大环之间的有效磁耦合3

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Neutral {CpFeII(CO)2[SnII(Pc?3?)]}{Cp iscyclopentadienyl(1,2) or Cp* is pentamethylcyclopentadienyl(3);Pc:phthalocyanine} ,{Cp*FeII(CO)2[SnII(Nc?3?)]}(4, Nc: naphthalocyanine),and {CpFeII(CO)2[SnII(TPP?3?)]} (5, TPP: tetraphenylporphyrin) complexes in which CpFeII(CO)2 fragments (Cp: Cpor Cp*) are coordinated to SnII(macrocycle?3?) have beenobtained. The product complexes were obtained at thereaction of charge transfer from CpFeI(CO)2 (Cp: Cp orCp*) to [SnII(macrocycle2?)] to form the diamagnetic FeII and paramagnetic radical trianionic macrocycles. As a result, theseformally neutral complexes contain S = 1/2 spins delocalized over the macrocycles. This provides alternation of the C?Nimine orC?Cmeso bonds in the macrocycles, the appearance of new bands in the near-infrared spectra of the complexes, and blue shift ofboth Soret and Q-bands. The {CpFeII(CO)2SnII(macrocycle?3?)} units (Cp: Cp or Cp*, macrocycle: Pc or Nc) form closelypacked π-stacking dimers in 1 and 3 or one-dimensional chains in 2 and 4 with effective π?π interaction between themacrocycles. Such packing allows strong antiferromagnetic coupling between S = 1/2 spins. Magnetic interaction can bedescribed well by the Heisenberg model for the isolated dimers in 1 and 3 with exchange interaction J/kB = ?78 and ?85 K,respectively. Magnetic behavior of 2 and 4 is described well by the model that includes contributions from anantiferromagnetically coupled S = 1/2 dimer (Jintra) and a Heisenberg S = 1/2 chain with alternating antiferromagnetic spinexchange between the neighbors (Jinter). Compound 2 demonstrates large intradimer interaction of Jintra/kB = ?54 K andessentially weaker interdimer exchange interactions of Jinter/kB = ?6 K, whereas compound 4 shows strong magnetic coupling ofspins within the dimers (Jintra/kB = ?170 K) as well as between the dimers (Jinter/kB = ?40 K). Compound{CpFeII(CO)2[SnII(TPP?3?)]} (5) shows no π?π interactions between the porphyrin macrocycles, and magnetic couplingis weak in this case (Weiss temperature is ?5 K). Preparation of a similar complex with indium(III) chloride phthalocyanineyields {CpFe(CO)2[In(Pc2?)]} (6). In this complex, indium(III) atoms are reduced instead of the phthalocyanine macrocyclesthat explains electron paramagnetic resonance silence of 6 in the 4?295 K range.
机译:中性{CpFeII(CO)2 [SnII(Pc?3?)]}} {Cp是环戊二烯基(1,2)或Cp *是五甲基环戊二烯基(3); Pc:酞菁},{Cp * FeII(CO)2 [SnII( Nc?3?)]}(4,Nc:萘酞菁)和{CpFeII(CO)2 [SnII(TPP?3?)]}}(5,TPP:四苯基卟啉)络合物,其中CpFeII(CO)2片段(Cp :已获得与SnII(大环?3?)配位的Cpor Cp *)。电荷从CpFeI(CO)2(Cp:Cp或Cp *)转移到[SnII(macrocycle2?)]形成顺磁性FeII和顺磁性自由基三阴离子大环化合物。结果,这些形式上中性的复合物包含在大环上离域的S = 1/2自旋。这提供了大环中C 3-亚胺或C 2 Cmeso键的交替,在复合物的近红外光谱中出现了新的谱带,以及Soret和Q谱带的蓝移。 {CpFeII(CO)2SnII(macrocycle?3?)}单元(Cp:Cp或Cp *,大环:Pc或Nc)在1和3中形成紧密堆积的π堆叠二聚体,或在2和4中形成一维链有效大环之间的π?π相互作用。这种堆积使得S = 1/2自旋之间具有强反铁磁耦合。磁相互作用可以通过Heisenberg模型很好地描述1和3中的分离二聚体,交换相互作用分别为J / kB =?78和?85K。该模型很好地描述了2和4的磁行为,该模型包括反铁磁耦合的S = 1/2二聚体(金特拉)和海森堡S = 1/2链(邻居之间交替发生反铁磁自旋交换)的贡献。化合物2显示出Jintra / kB =?54 K的大二聚体内部相互作用,而Jinter / kB =?6 K的二聚体之间的交换相互作用则弱得多,而化合物4也显示出二聚物内的自旋的强磁耦合(Jintra / kB =?170 K)。在二聚体之间(Jinter / kB =?40 K)。化合物{CpFeII(CO)2 [SnII(TPPα3α)]}(5)在卟啉大环之间没有παπ相互作用,在这种情况下磁耦合弱(Weiss温度为约5K)。制备具有氯化铟(III)酞菁的类似配合物,产率为{CpFe(CO)2 [In(Pc2?)]}(6)。在该络合物中,铟(III)原子被还原,而不是被酞菁大环还原,这解释了在4?295 K范围内6的电子顺磁共振沉默。

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