Zavoisky Physical-Technical Institute, FRC Kazan Scientific Center of RAS, Kazan, Russian Federation.
Department of Chemistry Brock University, St. Catharines, Ontario L2S 3A1, Canada.
J Chem Phys. 2019 Nov 14;151(18):184301. doi: 10.1063/1.5127762.
The light-induced electron spin polarization generated in the excited quartet and doublet states of a system consisting of a chromophore with an attached radical is investigated theoretically. Excitation of the chromophore and subsequent relaxation leads to a coupled triplet-doublet spin system. In many such systems, the electronic coupling between the triplet and doublet spins is expected to be strong enough to split the spin system into so-called trip-doublet and trip-quartet states but sufficiently weak that it does not promote significant mixing between the sing-doublet and trip-doublet states. In such moderately coupled systems, the sing-doublet can relax to the trip-doublet and trip-quartet states by spin-orbit coupling mediated intersystem crossing within the chromophore. An analytical expression is derived for the intensity of the polarization generated by this mechanism for the m = +1/2 ↔ -1/2 electron paramagnetic resonance transitions of the trip-doublet and trip-quartet states. The expression shows that the intensity and sign of the polarization depend strongly on ratio j = 3J/ω between the triplet-doublet exchange interaction J and the Zeeman energy ω. The polarization becomes undefined when j = 1 and when j = 2 because level-anticrossings between the trip-doublet and trip-quartet sublevels occur. The sign of the polarization is also found to change above and below these values. Thus, for such moderately coupled systems, the sign of the polarization and its Zeeman energy dependence can be used to estimate the magnitude of the exchange coupling.
本文理论研究了发色团与自由基相连的体系中激发的四重态和双重态中产生的光诱导电子自旋极化。发色团的激发和随后的弛豫导致耦合的三重态-双重态自旋系统。在许多这样的系统中,预计三重态和双重态之间的电子耦合足够强,足以将自旋系统分裂为所谓的三重态-双重态和三重态-四重态,但足够弱,不会促进单态-双重态和三重态-双重态之间的显著混合。在这种中等耦合的系统中,单态-双重态可以通过发色团内的自旋轨道耦合介导的体系间交叉弛豫到三重态-双重态和三重态-四重态。推导出了用于该机制产生的极化强度的解析表达式,用于三重态-双重态和三重态-四重态的 m = +1/2 ↔ -1/2 电子顺磁共振跃迁。该表达式表明,极化的强度和符号强烈依赖于三重态-双重态交换相互作用 J 和塞曼能 ω 之间的比值 j = 3J/ω。当 j = 1 和 j = 2 时,极化变得不确定,因为三重态-双重态和三重态-四重态亚能级之间发生能级交叉。还发现极化的符号在这些值之上和之下也会发生变化。因此,对于这种中等耦合的系统,极化的符号及其对塞曼能的依赖性可用于估计交换耦合的大小。