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Intersystem crossing mechanism of thermally activated delayed fluorescence copper(I) thiolate complex: The roles of exchange coupling and magnetic spin interactions
Organic Electronics ( IF 2.7 ) Pub Date : 2017-10-16 , DOI: 10.1016/j.orgel.2017.10.014
LingLing Lv , Kun Yuan , YongCheng Wang

The exchange coupling (J) and magnetic dipole (D) interactions of thermally activated delayed fluorescence copper(I) thiolate complex have been investigated by employing computational chemistry methods. The situation of strict orthogonality of the "hole”–“electron" orbitals with the overlap integral 〈ϕ175α|ϕ175β〉 = 0 leads to small J and excessive triplet T1 population, and is unfavorable to the formation of singlet S1 state via the exchange coupling induced reverse intersystem crossing in the triplet state T1. In magnetic dipole interactions, the mutually perpendicular orbitals provides a significant one-center heavy atomic contribution to the SOC, 〈1φ|hySO|3φ〉 = -41.76 and 〈1φ|hzSO|3φ〉 = −63.14 cm−1, which will enhance the probability of intersystem crossing from the T1 to S1, but system needs to overcome a large intersystem crossing barrier height of 11.05 kcal/mol relative to that of the T1 state at the CAM-B3LYP/def2-TZVP(-f) level. Under magnetic field limit, S1−T0, S1−T+1, and S1−T-1 mixing are all inefficient because the large energy gap between T1 and S1, |2J| » gβB prohibits significant mixing in the triplet state T1, but for the S1/T1 crossing point, the S1−T-1 energy gap is comparable to that of the S1−T0 energy gap, allowing for mixing of S1 with T-1 and T0, |Tz〉 = 56%|1, 0〉 + 20%|1, −1〉 + 16%|0, 0〉.



中文翻译:

热活化延迟荧光硫醇铜(I)配合物的系统间穿越机制:交换耦合和磁自旋相互作用的作用

采用计算化学方法研究了热活化的延迟荧光硫醇铜(I)配合物的交换偶合(J)和磁偶极(D)相互作用。的“洞”的严格正交性的情况-与重叠积分<“电子”轨道φ 175α | φ 175β > = 0导致小J和过度三重Ť 1人口,并且不利于形成单峰小号1通过交换状态耦合感应反向系间窜越的三重态T 1。在磁偶极子相互作用,在相互垂直的轨道提供给SOC一个显著一个中心重原子贡献,< 1个φ | ^ h ÿ SO | 3 φ > = -41.76和< 1个φ | h z SO | 3 φ > = -63.14厘米-1,这将提高系间窜越的概率从T 1至S 1,但系统的需求,以克服11.05大间跨越势垒高度千卡/摩尔相对于T形1状态在CAM-B3LYP / def2-TZVP(-f)级别上。在磁场极限下,S 1-T 0,S 1 -T +1和S 1 -T -1混合均无效,因为T 1与S 1之间的能隙较大,| 2 J |。» gβB禁止在三重态T 1中进行显着混合,但对于S 1 / T 1交叉点,S 1 -T -1的能隙与S 1 -T 0的能隙相当,从而允许混合具有T -1和T 0的| S 1,| T z〉 = 56%| 1,0〉 + 20%| 1,-1〉 + 16%| 0,0〉。

更新日期:2017-10-16
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